1 UI - 14713 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Balm PW AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Begel M AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Besson A AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buehler M AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Canelli F AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Cho DK AU - Choi S AU - Chopra S AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis GA AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Demina R AU - Demine P AU - Denisov D AU - Denisov SP AU - Desai S AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Doulas S AU - Draper P AU - Ducros Y AU - Dudko LV AU - Duensing S AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Graham G AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Groer L AU - Grudberg P AU - Grunendahl S AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hou S AU - Huang Y AU - Ito AS AU - Jerger SA AU - Jesik R AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Kuznetsov VE AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn S AU - Linnemann J AU - Lipton R AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mao HS AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McMahon T AU - Melanson HL AU - Meng XC AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Moore RW AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AD - Univ Buenos Aires, RA-1053 Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaCharles Univ, Prague, Czech RepublicUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Sci Nucl, F-38041 Grenoble, FranceUniv Mediterranee, CNRS, IN2P3, CPPM, Marseille, FranceUniv Paris 05, LPNHE, CNRS, IN2P3, Paris, FranceUniv Paris 07, LPNHE, CNRS, IN2P3, Paris, FranceCEA Saclay, Serv Phys Particules, DAPNIA, F-91191 Gif Sur Yvette, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi, IndiaTata Inst Fundamental Res, Bombay 400005, Maharashtra, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoNIKHEF H, FOM, NL-1009 DB Amsterdam, NetherlandsUniv Amsterdam, NIKHEF H, Amsterdam, NetherlandsInst Phys Nucl, Krakow, PolandMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster LA1 4YW, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USANYU, New York, NY 10003, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, Univ Buenos Aires, RA-1053 Buenos Aires, DF, Argentina TI - Cross section for b-jet production in (p)over-barp collisions at root s=1.8 TeV AB - Bottom-quark production in (p) over barp collisions at roots = 1.8 TeV is studied with 5 pb(-1) of data collected in 1995 by the DO detector at the Fermilab Tevatron Collider The differential production cross section for b jets in the central rapidity region (\y(b)\ < 1) as a function of jet transverse energy is extracted from a muon-tagged jet sample. Within experimental and theoretical uncertainties, DO results are found to be higher than, but compatible with, next-to-leading-order QCD predictions MH - Argentina MH - Brazil MH - Colombia MH - Czech Republic MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Netherlands MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 44 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000165800000014 L2 - HEAVY QUARK PRODUCTION; P(P)OVER-BAR COLLISIONS; HADRONIC COLLISIONS; E+E ANNIHILATION; QCD SO - Physical Review Letters 2000 ;85(24):5068-5073 2 UI - 14912 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Begel M AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Besson A AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buehler M AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Canelli F AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis GA AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Demina R AU - Demine P AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Doulas S AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Filthaut F AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Ito AS AU - Jerger SA AU - Jesik R AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Kuznetsov V AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McMahon T AU - Melanson HL AU - Meng XC AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AU - Patwa A AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaCharles Univ, Prague, Czech RepublicAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicUniv San Francisco, Quito, EcuadorUniv Grenoble 1, Inst Sci Nucl, CNRS, IN2P3, Grenoble, FranceUniv Mediterranee, CPPM, CNRS, IN2P3, Marseille, FranceUniv Paris 06, LPNHE, CNRS, IN2P3, Paris, FranceUniv Paris 07, LPNHE, CNRS, IN2P3, Paris, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoUniv Nijmegen, NIKHEF, Nijmegen, NetherlandsInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Search for new physics in e mu X data at DO using SLEUTH: A quasi-model-independent search strategy for new physics AB - We present a quasi-model-independent search for the physics responsible for electroweak symmetry breaking. We define final states to be studied, and construct a rule that identifies a set of relevant variables for any particular final state. A new algorithm ("SLEUTH") searches for regions of excess in those variables and quantifies the significance of any detected excess. After demonstrating the sensitivity of the method, we apply it to the semi-inclusive channel e muX collected in 108 pb(-1) of p(p) over bar collisions at roots=1.8 TeV at the DO experiment during 1992-1996 at the Fermilab Tevatron. We find no evidence of new high p(T) physics in this sample MH - Argentina MH - Brazil MH - Colombia MH - Czech Republic MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Netherlands MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 9 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000165111400008 L2 - DYNAMICAL SYMMETRY BREAKING; PRODUCTION CROSS-SECTION; TOP-QUARK SEARCH; P(P)OVER-BAR COLLISIONS; SUPERSYMMETRY; FERMILAB; NEUTRALINOS; CHARGINOS; ENERGY; DECAYS SO - Physical Review D 2000 ;6209(9): 3 UI - 14913 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adam I AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Belyaev A AU - Beri SB AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Bloom P AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Boswell C AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Cooper WE AU - Coppage D AU - Cretsinger C AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Forden GE AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Geld TL AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Hernandez-Montoya R AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Hu T AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Madden R AU - Magana-Mendoza L AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nang F AU - Narain M AU - Narasimham VS AU - Narayanan A AU - Neal HA AU - Negret JP AU - Nemethy P AU - Norman D AU - Oesch L AU - Oguri V AU - Oshima N AU - Owen D AU - Padley P AU - Para A AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janiero, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco, Quito, EcuadorUniv Grenoble 1, Inst Sci Nucl, CNRS, IN2P3, Grenoble, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaKyungsung Univ, Pusan 608736, South KoreaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAAbbott, B, NYU, New York, NY 10003, USA TI - Measurement of the W boson mass using large rapidity electrons AB - \We present a measurement of the W boson mass using data collected by the DO experiment at the Fermilab Tevatron during 1994-1995. We identify W bosons by their decays to ev final states where the electron is detected in a forward calorimeter. We extract the W boson mass M-W by fitting the transverse mass and transverse electron and neutrino momentum spectra from a sample of 11 089 W-->e nu decay candidates. We use a sample of 1687 dielectron events, mostly due to Z-->ee decays, to constrain our model of the detector response. Using the forward calorimeter data, we measure M-w=80.691+/-0.227 GeV. Combining the forward calorimeter measurements with our previously published central calorimeter results, we obtain M-W= 80.482 +/-0.091 GeV MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 13 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000165111400010 L2 - TOP-QUARK MASS; CTEQ PARTON DISTRIBUTIONS; QED RADIATIVE-CORRECTIONS; CERN PBARP COLLIDER; P(P)OVER-BAR COLLISIONS; TRANSVERSE-MOMENTUM; FERMILAB-TEVATRON; STANDARD MODEL; D0 DETECTOR; NUCLEON SEA SO - Physical Review D 2000 ;6209(9): 4 UI - 15069 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buehler M AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Canelli F AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Doulas S AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McMahon T AU - Melanson HL AU - Meng XC AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AU - Patwa A AU - Pawlik B AU - Perkins J AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaCharles Univ, Prague, Czech RepublicAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Sci Nucl, Grenoble, FranceUniv Mediterranee, CNRS, IN2P3, CPPM, Marseille, FranceUniv Paris 06, LPNHE, CNRS, IN2P3, Paris, FranceUniv Paris 07, LPNHE, CNRS, IN2P3, Paris, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Phys Nucl, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Berkeley, CA 94720, USALawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47408, USAUniv Notre Dame, Notre Dame, IN 46556, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Search for R-parity violation in multilepton final states in p(p)over-bar collisions at root s=1.8 TeV AB - The result of a search for gaugino pair production with a trilepton signature is reinterpreted in the framework of minimal supergravity (MSUGRA) with R-parity violation via leptonic lambda Yukawa couplings. The search used 95 pb(-1) of p (p) over bar collisions at root s = 1.8 TeV recorded by the D empty set detector at the Fermilab Tevatron. A large domain of the MSUGRA parameter space is excluded for lambda(121), lambda(122)greater than or equal to 10(-4) MH - Argentina MH - Brazil MH - Colombia MH - Czech Republic MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 8 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000089749400005 L2 - GRAND UNIFICATION; TOP-QUARK; SUPERSYMMETRY; SUPERGRAVITY; MASS SO - Physical Review D 2000 ;6207(7): 5 UI - 15301 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buehler M AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Canelli F AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Doulas S AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McMahon T AU - Melanson HL AU - Meng XC AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AU - Patwa A AU - Pawlik B AU - Perkins J AD - Univ Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio De Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaCharles Univ, Prague, Czech RepublicAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicUniv San Francisco, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Nucl Sci, Grenoble, FranceUniv Mediterranee, CNRS, IN2P3, CPPM, Marseille, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceCEA Saclay, Serv Phys Particules, DAPNIA, F-91190 Gif Sur Yvette, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Bombay 400005, Maharashtra, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USANYU, New York, NY 10003, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, Univ Buenos Aires, Buenos Aires, DF, Argentina TI - The b(b)over-bar production cross section and angular correlations in p(p)over-bar collisions at root s = 1.8 TeV AB - We present measurements of the b (b) over bar production cross section and angular correlations using the D phi detector at the Fermilab Tevatron p (p) over bar Collider operating at root s = 1.8 TeV. The b quark production cross section for /y(b)/ < 1.0 and P-T(b) > 6 GeV/c is extracted from the single muon and dimuon data samples. The results agree in shape with me next-to-leading order QCD calculation of heavy flavor production but are greater than the central values of these predictions. The angular correlations between b and (b) over bar quarks, measured from the azimuthal opening angle between their decay muons, also agree in shape with the next-to-leading order QCD prediction. (C) 2000 Elsevier Science B.V. All rights reserved MH - Argentina MH - Brazil MH - Colombia MH - Czech Republic MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - AMSTERDAM: ELSEVIER SCIENCE BV RP - NOT IN FILE U3 - TC 62 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0370-2693 UR - ISI:000089046600007 L2 - ROOT-S=1.8 TEV; QUARK PRODUCTION; COLLIDER SO - Physics Letters B 2000 ;487(3-4):264-272 6 UI - 15330 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Cheliulaev SV AU - Chen LP AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Gonchalrov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritski AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, Inst Sci Nucl, CNRS, IN2P3, Grenoble, FranceCtr Phys Particules Marseille, CNRS, IN2P3, Marseille, FranceUniv Paris 06, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, Paris, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Limits on anomalous WW gamma and WWZ couplings from WW/WZ -> evjj production AB - Limits on anomalous WW gamma and WWZ couplings are presented from a study of WW/WZ-->evjj events produced in p (p) over bar collisions at root s=1.8 TeV. Results from the analysis of data collected using the DO detector during the 1993-1995 Tevatron collider run at Fermilab are combined with those of an earlier study from the 1992-1993 run. A fit to the transverse momentum spectrum of the W boson yields direct limits on anomalous WW gamma and WWZ couplings. With the assumption that the WW gamma and WWZ couplings are equal, we obtain -0.34 < lambda < 0.36 (with Delta kappa = 0) and -0.43 < Delta kappa < 0.59 (with lambda = 0) at the 95% confidence level for a form-factor scale Lambda = 2.0 TeV MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 13 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000089022500009 L2 - GAUGE-BOSON COUPLINGS; ALPHA-S CALCULATION; ROOT-S=1.8 TEV; P(P)OVER-BAR COLLISIONS; FERMILAB-TEVATRON; PAIR PRODUCTION; WZ PRODUCTION; W+W PRODUCTION; D0 DETECTOR; COLLIDER SO - Physical Review D 2000 ;6205(5): 7 UI - 15544 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buehler M AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Canelli F AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Doulas S AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelman R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McMahon T AU - Melanson HL AU - Meng XC AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AU - Patwa A AU - Pawlik B AU - Perkins J AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaCharles Univ, Prague, Czech RepublicAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicUniv San Francisco, Quito, EcuadorUniv Grenoble 1, CNRS, Inst Sci Nucl, IN2P3, Grenoble, FranceUniv Mediterranee, CPPM, CNRS, IN2P3, Marseille, FranceUniv Paris 06, LPNHE, Paris, FranceUniv Paris 07, IN2P3, CNRS, Paris, FranceCEA, DAPNIA, Serv Phys Particules, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow MV Lomonosov State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USANYU, New York, NY 10003, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Limits on quark compositeness from high energy jets in (p)over-bar-p collisions at 1.8 TeV AB - Events in (p) over bar p collisions at root s = 1.8 TeV with total transverse energy exceeding 500 GeV are used to set limits on quark substructure. The data are consistent with next-to-leading order QCD calculations. We set a lower limit of 2.0 TeV at 95% confidence on the energy scale Lambda(LL) for compositeness in quarks. assuming a model with a left-left isoscalar contact interaction term. The limits on Lambda(LL) are found to be insensitive to the sign of the interference term in the Lagrangian MH - Argentina MH - Brazil MH - Colombia MH - Czech Republic MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 5 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000088516300001 L2 - DIJET ANGULAR-DISTRIBUTIONS; CROSS-SECTION; PARTON DISTRIBUTIONS; GLOBAL ANALYSIS; ROOT-S=1.8TEV; DETECTOR; PHYSICS; SEARCH SO - Physical Review D 2000 ;6203(3): 8 UI - 15659 AU - Abbott B AU - Abramov MAV AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Bueschre V AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Ri de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Nucl Sci, Grenoble, FranceUniv Mediterranee, CNRS, IN2P3, CPPM, Marseille, FranceUniv Paris 06, LPHNE, Paris, FranceUniv Paris 07, CNRS, IN2P3, Paris, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Bombay 400005, Maharashtra, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USALawrence Berkeley Natl Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Spin correlation in t(t)over-bar production from p(p)over-bar collisions at root s=1.8 TeV AB - The D0 collaboration has performed a study of spin correlation in t (t) over tilde production for the process t (t) over bar --> bW(+)(b) over bar W-, where the W bosons decay to e nu or mu nu. A sample of six events was collected during an exposure of the DO detector to an integrated luminosity of approximately 125 pb(-1) of root s = 1.8 TeV p (p) over bar collisions. The standard model (SM) predicts that the short lifetime of the top quark ensures the transmission of any spin information at production to the t (t) over bar decay products. The degree of spin correlation is characterized by a correlation coefficient kappa. We find that kappa > -0.25 at the 68% confidence level. in agreement with the SM prediction of kappa = 0.88 MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 20 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000088048700008 L2 - TOP-QUARK PAIR; PRODUCTION CROSS-SECTION; ART. NO. 052001; COLLIDER DETECTOR; E(+)E(-) COLLIDERS; HADRON COLLIDERS; DILEPTON EVENTS; DECAY; MASS; FERMILAB SO - Physical Review Letters 2000 ;85(2):256-261 9 UI - 15807 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassier U AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad S AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li H AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AD - NYU, New York, NY 10003, USAColumbia Univ, New York, NY 10027, USAUniv Nebraska, Lincoln, NE 68588, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Michigan, Ann Arbor, MI 48109, USANortheastern Univ, Boston, MA 02115, USABoston Univ, Boston, MA 02215, USAUniv Maryland, College Pk, MD 20742, USALouisiana Tech Univ, Ruston, LA 71272, USAKansas State Univ, Manhattan, KS 66506, USAUniv Kansas, Lawrence, KS 66045, USAIowa State Univ Sci & Technol, Ames, IA 50011, USAPurdue Univ, W Lafayette, IN 47907, USAUniv Notre Dame, Notre Dame, IN 46556, USAIndiana Univ, Bloomington, IN 47405, USANorthwestern Univ, Evanston, IL 60208, USANo Illinois Univ, De Kalb, IL 60115, USAUniv Illinois, Chicago, IL 60607, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Hawaii, Honolulu, HI 96822, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Calif Riverside, Riverside, CA 92521, USAUniv Calif Irvine, Irvine, CA 92697, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Arizona, Tucson, AZ 85721, USAUniv Lancaster, Lancaster, EnglandInst High Energy Phys, Protvino, RussiaInst Nucl Phys, Krakow, PolandCINVESTAV, Mexico City 14000, DF, MexicoSeoul Natl Univ, Seoul, South KoreaTata Inst Fundamental Res, Mumbai, IndiaUniv Delhi, Delhi 110007, IndiaPanjab Univ, Chandigarh 160014, IndiaMoscow State Univ, Moscow, RussiaInst Theoret & Expt Phys, Moscow 117259, RussiaCEA, DAPNIA, Serv Phys Particules, Saclay, FranceUniv Paris 06, CNRS, LPHNE, IN2P3, Paris, FranceUniv Paris 07, CNRS, LPHNE, IN2P3, Paris, FranceUniv Grenoble 1, CNRS, IN2P3, Inst Nucl Sci, Grenoble, FranceUniv San Francisco, Quito, EcuadorUniv Los Andes, Bogota, ColombiaInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Buenos Aires, Buenos Aires, DF, ArgentinaUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Measurement of the W ->tau nu production cross section in p(p)over-bar collisions at root s=1.8 TeV AB - of data collected with the DO detector during 1993-1995. We find that a(p (p) over bar --> W + X)B(W --> tau nu) = 2.22 +/- 0.09 (stat) +/- 0.10 (syst) +/- 0.10 (lum) nb. Lepton universality predicts that the ratio of the tau and electron electroweak charged current couplings to the W boson, g(T)(W)/g(e)(W), be unity. We find g(T)(W)/g(e)(W) = 0.980 +/- 0.031, in agreement with lepton universality MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 4 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000087653300007 L2 - E(+)E(-) INTERACTIONS; BRANCHING FRACTIONS; PAIR PRODUCTION; COLLIDER; DECAY SO - Physical Review Letters 2000 ;84(25):5710-5715 10 UI - 15808 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Bean A AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Juste A AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mihalcea D AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Padley P AU - Pan LJ AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AU - Patwa A AU - Pawlik B AD - NYU, New York, NY 10003, USAColumbia Univ, New York, NY 10027, USAUniv Nebraska, Lincoln, NE 68588, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Michigan, Ann Arbor, MI 48109, USANortheastern Univ, Boston, MA 02115, USABoston Univ, Boston, MA 02215, USAUniv Maryland, College Pk, MD 20742, USALouisiana Tech Univ, Ruston, LA 71272, USAKansas State Univ, Manhattan, KS 66506, USAUniv Kansas, Lawrence, KS 66045, USAIowa State Univ Sci & Technol, Ames, IA 50011, USAUniv Notre Dame, Notre Dame, IN 46556, USAIndiana Univ, Bloomington, IN 47405, USANorthwestern Univ, Evanston, IL 60208, USANo Illinois Univ, De Kalb, IL 60115, USAUniv Illinois, Chicago, IL 60607, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Hawaii, Honolulu, HI 96822, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Calif Riverside, Riverside, CA 92521, USAUniv Calif Irvine, Irvine, CA 92697, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Arizona, Tucson, AZ 85721, USAUniv Lancaster, Lancaster, EnglandInst High Energy Phys, Protvino, RussiaMoscow MV Lomonosov State Univ, Moscow, RussiaInst Theoret & Expt Phys, Moscow 117259, RussiaInst Nucl Phys, Krakow, PolandCINVESTAV, Mexico City 14000, DF, MexicoSeoul Natl Univ, Seoul, South KoreaTata Inst Fundamental Res, Mumbai, IndiaUniv Delhi, Delhi 110007, IndiaPanjab Univ, Chandigarh 160014, IndiaCEA, DAPNIA, Serv Phys Particules, Saclay, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceUniv Mediterranee, CNRS, IN2P3, CPPM, Marseille, FranceUniv Grenoble 1, CNRS, IN2P3, Inst Sci Nucl, Grenoble, FranceUniv San Francisco, Quito, EcuadorUniv Los Andes, Bogota, ColombiaInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Estado Rio Janeiro, Rio De Janeiro, BrazilCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Buenos Aires, Buenos Aires, DF, ArgentinaUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Probing Balitsky-Fadin-Kuraev-Lipatov dynamics in the dijet cross section at large rapidity intervals in p(p)over-bar collisions at root s=1800 and 630 GeV AB - Inclusive dijet production at large pseudorapidity intervals (Delta eta) between the two jets has been suggested as a regime for observing Balitsky-Fadin-Kuraev-Lipatov (BFKL) dynamics. We have measured the dijet cross section for large Delta eta in p (p) over bar collisions at root s = 1800 and 630 GeV using the D0 detector. The partonic cross section increases strongly with the size of Delta eta; The observed growth is even stronger than expected on the basis of BFKL resummation in the leading logarithmic approximation. The growth of the partonic cross section can be accommodated with an effective BFKL intercept of alpha(BFKL)(20 GeV) = 1.65 +/- 0.07 MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 19 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000087653300009 L2 - DEEP-INELASTIC SCATTERING; JET PRODUCTION; HERA; ENERGY; SINGULARITY; POMERON; MESON SO - Physical Review Letters 2000 ;84(25):5722-5727 11 UI - 15860 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adam I AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Belyaev A AU - Beri SB AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Bloom P AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Boswell C AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Cooper WE AU - Coppage D AU - Cretsinger C AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Forden GE AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Geld TL AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Hernandez-Montoya R AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Hu T AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Madden R AU - Magana-Mendoza L AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nang F AU - Narain M AU - Narasimham VS AU - Narayanan A AU - Neal HA AU - Negret JP AU - Nemethy P AU - Norman D AU - Oesch L AU - Oguri V AU - Oshima N AU - Owen D AU - Padley P AU - Para A AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio De Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Nucl Sci, Grenoble, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Bombay 400005, Maharashtra, IndiaKyungsung Univ, Pusan 608736, South KoreaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USALawrence Berkeley Natl Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAAbbott, B, NYU, 550 1St Ave, New York, NY 10003, USA TI - Small-angle muon and bottom-quark production in p(p)over-bar collisions at root s=1.8 TeV AB - This Letter describes a measurement of the muon cross section originating from b-quark decay in the forward rapidity range 2.4 < \y(mu)\ < 3.2 in p (p) over bar collisions at root s = 1.8 TeV. The data used in this analysis were collected by the DO experiment at the Fermilab Tevatron. We find that next-to-leading-order QCD calculations underestimate b-quark production by a factor of 4 in the forward rapidity region MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 18 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000087522200006 L2 - = 1.8 TEV; DIFFERENTIAL CROSS-SECTION; P(P)OVER-BAR COLLISIONS; HADRON-COLLISIONS; D0 DETECTOR; DISTRIBUTIONS SO - Physical Review Letters 2000 ;84(24):5478-5483 12 UI - 16258 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adam I AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Belyaev A AU - Beri SB AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Bloom P AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Boswell C AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chekulaev SV AU - Chen W AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Cooper WE AU - Coppage D AU - Cretsinger C AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Forden GE AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Geld TL AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Hernandez-Montoya R AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Hu T AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Jung CK AU - Kahn S AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Madden R AU - Magana-Mendoza L AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Murphy C AU - Nang F AU - Narain M AU - Narasimham VS AU - Narayanan A AU - Neal HA AU - Negret JP AU - Nemethy P AU - Norman D AU - Oesch L AU - Oguri V AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Park YM AU - Partridge R AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Sci Nucl, Grenoble, FranceCEA Saclay, Serv Phys Particules, DAPNIA, Gif Sur Yvette, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaKyungsung Univ, Pusan 608736, South KoreaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USALawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USANYU, New York, NY 10003, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAAbbott, B, NYU, New York, NY 10003, USA TI - Extraction of the width of the W boson from measurements of sigma(p(p)over-bar -> W+X) x B(W -> e nu) and sigma(p(p)over-bar -> Z+X) x B(Z -> ee) and their ratio AB - We report on measurements on inclusive cross sections times branching fractions into electrons for W and Z bosons produced in p (p) over bar collisions at root s = 1.8 TeV. From an integrated luminosity of 84.5 pb(-1) recorded in 1994-1995 using the D empty set detector at the Fermilab Tevatron, we determine sigma(p (p) over bar--> W + X) x B(W-->e nu) = 2310 +/- 10(stat) +/- 50(syst) +/- 100(lum)pb and sigma(p (p) over bar-->Z + X) x B(Z-->ee)=221+/-3(stat)+/-4(syst)+/-10(lum)pb. From these, we derive sigma(p (p) over bar-->W + X) x B(N-->e nu)/sigma(p (p) over bar-->Z + X) x B(Z-->ee) = 10.43+/-0.15(stat) +/- 0.20(syst) +/- 0.10(NLO), B(W-->e nu) = 0.1044+/-0.0015(stat)+/-0.0020(syst)+/-0.0017(theory)+/-0.0010(NLO). and Gamma(w) = 2169 +/- 0.03 l(stat) +/- 0.042(syst) +/- 0.041(theory)+/- 0.022(NLO)GeV. We use the latter to set a 95% confidence level upper limit on the partial decay width of the W boson into nonstandard model final states, Gamma(W)(inv), of 0.213 GeV. Combining these results with those from the 1992-1993 data gives sigma(p (p) over bar-->W+X) x B(W-->e nu)/sigma(p (p) over bar-->Z+X) x B(Z-->ee) = 10.51+/-0.25, Gamma(W) = 2.152 +/- 0.066 GeV, and a 95% C.L. upper limit an Gamma(W)(inv) of 0.191 GeV. Using a sample with a luminosity of 505 nb(-1) taken at root s = 630 GeV, we measure sigma(p (p) over bar--> W+ X) x B(W --> e nu) = 658 +/- 67 pb MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 31 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000086065200009 L2 - CTEQ PARTON DISTRIBUTIONS; CERN PBARP COLLIDER; YAN K-FACTOR; ROOT-S=1.8 TEV; P(P)OVER-BAR COLLISIONS; GAMMA COUPLINGS; CROSS-SECTIONS; E(+)E(-) INTERACTIONS; TRANSVERSE-MOMENTUM; PAIR-PRODUCTION SO - Physical Review D 2000 ;6107(7): 13 UI - 16307 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Buescher V AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugas SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HW AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landsberg G AU - Leflat A AU - Lehner F AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Lundstedt C AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Mattin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier B AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Partridge R AU - Parua N AU - Paterno M AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Nucl Sci, Grenoble, FranceCtr Phys Particules Marseille, CNRS, IN2P3, Marseille, FranceUniv Paris 06, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, Paris, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USALawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, New York, NY 10003, USA TI - Isolated photon cross section in p(p)over-bar collisions at root s=1.8 TeV AB - We report a new measurement of the cross section for the production of isolated photons with transverse energies (E-T(gamma)) above 10 GeV and pseudorapidities \eta\ < 2.5 in p (p) over bar collisions at root s = 1.8 TeV. The results are based on a data sample of 107.6 pb(-1) recorded during 1992-1995 with the D0 detector at the Fermilab Tevatron collider. The background, predominantly from jets which fragment to neutral mesons, was estimated using the longitudinal shower shape of photon candidates in the calorimeter. The measured cross section is in good agreement with the next-to-leading order QCD calculation for E-T(gamma) greater than or similar to 36 GeV MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 32 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000086062000006 SO - Physical Review Letters 2000 ;84(13):2786-2791 14 UI - 16308 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adam I AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Belyaev A AU - Beri SB AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Bloom P AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Boswell C AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Cooper WE AU - Coppage D AU - Cretsinger C AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Forden GE AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Geld TL AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Hernandez-Montoya R AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen N AU - Hoftun JS AU - Hsieh F AU - Hu T AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffi-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Madden R AU - Magana-Mendoza L AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nang F AU - Narain M AU - Narasimham VS AU - Narayanan A AU - Neal HA AU - Negret JP AU - Nemethy P AU - Norman D AU - Oesch L AU - Oguri V AU - Oshima N AU - Owen D AU - Padley P AU - Para A AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Sci Nucl, Grenoble, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaKyungsung Univ, Pusan 608736, South KoreaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster LA1 4YW, EnglandUniv Arizona, Tucson, AZ 85721, USALawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAAbbott, B, NYU, New York, NY 10003, USA TI - Differential production cross section of Z bosons as a function of transverse momentum at root s=1.8 TeV AB - We present a measurement of the transverse momentum distribution of Z bosons produced in p (p) over bar collisions at root s = 1.8 TeV from data collected by the DO experiment at the Fermilab Tevatron Collider, We find good agreement between our results and current resummation calculations, and also use our data to extract nonperturbative parameters for a particular version of the resummation formalism. The resulting values are significantly more precise than obtained in previous determinations MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 13 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000086062000007 L2 - MONTE-CARLO; W-BOSON; COLLIDERS; QCD SO - Physical Review Letters 2000 ;84(13):2792-2797 15 UI - 16422 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Bassler U AU - Belyaev A AU - Beri SB AU - Bernardi G AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Brooijmans G AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fleuret F AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NH AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nagy E AU - Nang F AU - Narain M AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Negroni S AU - Norman D AU - Oesch L AU - Oguri V AU - Olivier R AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Partridge R AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaLAFEX, Ctr Brasileiro Pesquisas Fis, Rio De Janeiro, BrazilUniv Estado Rio De Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, CNRS, IN2P3, Inst Sci Nucl, Grenoble, FranceCNRS, IN2P3, Ctr Phys Particules Marseillo, Marseille, FranceUniv Paris 06, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, Paris, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Bombay 400005, Maharashtra, IndiaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USALawrence Berkeley Natl Lab, Berkeley, CA 94720, USAUniv Calif Berkeley, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USACalif State Univ Fresno, Fresno, CA 93740, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, NYU, 550 1St Ave, New York, NY 10003, USA TI - Search for second-generation leptoquark pairs in (p)over-barp collisions at root s=1.8 TeV AB - We have searched for second-generation leptoquark (LQ) pairs in the mu mu + jets channel using 94 +/- 5 pb(-1) of (p) over bar p collider data collected by the DO experiment at the Fermilab Tevatron during 1993-1996. No evidence for a signal is observed. These results are combined with those from the mu v + jets and vv + jets channels to obtain 95% confidence level (C.L.) upper limits on the LQ pair production cross section as a function of mass and beta, the branching fraction of a LQ decay into a charged lepton and a quark. Lower limits of 200(180) GeV/c(2) for beta = 1(1/2) are set at the 95% C.L. on the mass of scalar LQ. Mass limits are also set on vector leptoquarks as a function of beta MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 28 U4 - Physics, Multidisciplinary U5 - J;Article AV - English IS - 0031-9007 UR - ISI:000085650100011 L2 - P(P)OVER-BAR COLLISIONS SO - Physical Review Letters 2000 ;84(10):2088-2093 16 UI - 16546 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adam I AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsey VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Belyaev A AU - Beri SB AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Bloom P AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Boswell C AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chekulaev SV AU - Chen W AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Cooper WE AU - Coppage D AU - Cretsinger C AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein D AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Forden GE AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Geld TL AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard B AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon H AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez P AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn KS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Hernandez-Montoya R AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Hu T AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Jung CK AU - Kahn S AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Madden R AU - Magana-Mendoza L AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Murphy C AU - Nang F AU - Narain M AU - Narasimham VS AU - Narayanan A AU - Neal HA AU - Negret JP AU - Nemethy P AU - Norman D AU - Oesch L AU - Oguri V AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Park YM AU - Partridge R AD - NYU, New York, NY 10003, USAUniv Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, Inst Sci Nucl, CNRS, IN2P3, Grenoble, FranceCEA, Serv Phys Particules, DAPNIA, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaKyungsung Univ, Pusan 608736, South KoreaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAAbbott, B, NYU, New York, NY 10003, USA TI - Measurement of the inclusive differential cross section for Z bosons as a function of transverse momentum in (p) over-barp collisions at root s=1.8 TeV AB - We present a measurement of the differential cross section as a function of transverse momentum of the Z boson in
collisions at root s = 1.8 TeV using data collected by the DO experiment at the Fermilab Tevatron Collider during 1994-1996. We find good agreement between our data and the next-to-next-to-next-leading-logarithmic resummation prediction and extract values of the non-perturbative parameters for the resummed prediction from a fit to the differential cross section MH - Argentina MH - Brazil MH - Colombia MH - Ecuador MH - United Kingdom MH - France MH - India MH - Mexico|Distrito Federal MH - Peoples R China MH - Poland MH - Russia MH - South Korea MH - USA PB - COLLEGE PK: AMERICAN PHYSICAL SOC RP - NOT IN FILE U3 - TC 22 U4 - Astronomy & Astrophysics;Physics, Particles & Fields U5 - J;Article AV - English IS - 0556-2821 UR - ISI:000085079600007 L2 - = 1.8 TEV; W-BOSON; PBARP COLLISIONS; LEPTON PAIRS; MONTE-CARLO; MASS; DISTRIBUTIONS; COLLIDERS; ENERGY; QCD SO - Physical Review D 2000 ;6103(3): 17 UI - 16651 AU - Abbott B AU - Abolins M AU - Abramov V AU - Acharya BS AU - Adam I AU - Adams DL AU - Adams M AU - Ahn S AU - Akimov V AU - Alves GA AU - Amos N AU - Anderson EW AU - Baarmand MM AU - Babintsev VV AU - Babukhadia L AU - Baden A AU - Baldin B AU - Banerjee S AU - Bantly J AU - Barberis E AU - Baringer P AU - Bartlett JF AU - Belyaev A AU - Beri SB AU - Bertram I AU - Bezzubov VA AU - Bhat PC AU - Bhatnagar V AU - Bhattacharjee M AU - Blazey G AU - Blessing S AU - Boehnlein A AU - Bojko NI AU - Borcherding F AU - Brandt A AU - Breedon R AU - Briskin G AU - Brock R AU - Bross A AU - Buchholz D AU - Burtovoi VS AU - Butler JM AU - Carvalho W AU - Casey D AU - Casilum Z AU - Castilla-Valdez H AU - Chakraborty D AU - Chan KM AU - Chekulaev SV AU - Chen W AU - Cho DK AU - Choi S AU - Chopra S AU - Choudhary BC AU - Christenson JH AU - Chung M AU - Claes D AU - Clark AR AU - Cobau WG AU - Cochran J AU - Coney L AU - Connolly B AU - Cooper WE AU - Coppage D AU - Cullen-Vidal D AU - Cummings MAC AU - Cutts D AU - Dahl OI AU - Davis K AU - De K AU - Del Signore K AU - Demarteau M AU - Denisov D AU - Denisov SP AU - Diehl HT AU - Diesburg M AU - Di Loreto G AU - Draper P AU - Ducros Y AU - Dudko LV AU - Dugad SR AU - Dyshkant A AU - Edmunds D AU - Ellison J AU - Elvira VD AU - Engelmann R AU - Eno S AU - Eppley G AU - Ermolov P AU - Eroshin OV AU - Estrada J AU - Evans H AU - Evdokimov VN AU - Fahland T AU - Fatyga MK AU - Feher S AU - Fein B AU - Ferbel T AU - Fisk HE AU - Fisyak Y AU - Flattum E AU - Fortner M AU - Frame KC AU - Fuess S AU - Gallas E AU - Galyaev AN AU - Gartung P AU - Gavrilov V AU - Genik RJ AU - Genser K AU - Gerber CE AU - Gershtein Y AU - Gibbard P AU - Gilmartin R AU - Ginther G AU - Gobbi B AU - Gomez B AU - Gomez G AU - Goncharov PI AU - Solis JLG AU - Gordon P AU - Goss LT AU - Gounder K AU - Goussiou A AU - Graf N AU - Grannis PD AU - Green DR AU - Green JA AU - Greenlee H AU - Grinstein S AU - Grudberg P AU - Grunendahl S AU - Guglielmo G AU - Guida JA AU - Guida JM AU - Gupta A AU - Gurzhiev SN AU - Gutierrez G AU - Gutierrez A AU - Hadley NJ AU - Haggerty H AU - Hagopian S AU - Hagopian V AU - Hahn HS AU - Hall RE AU - Hanlet P AU - Hansen S AU - Hauptman JM AU - Hays C AU - Hebert C AU - Hedin D AU - Heinson AP AU - Heintz U AU - Hernandez-Montoya R AU - Heuring T AU - Hirosky R AU - Hobbs JD AU - Hoeneisen B AU - Hoftun JS AU - Hsieh F AU - Ito AS AU - Jerger SA AU - Jesik R AU - Joffe-Minor T AU - Johns K AU - Johnson M AU - Jonckheere A AU - Jones M AU - Jostlein H AU - Jun SY AU - Kahn S AU - Kajfasz E AU - Karmanov D AU - Karmgard D AU - Kehoe R AU - Kim SK AU - Klima B AU - Klopfenstein C AU - Knuteson B AU - Ko W AU - Kohli JM AU - Koltick D AU - Kostritskiy AV AU - Kotcher J AU - Kotwal AV AU - Kozelov AV AU - Kozlovsky EA AU - Krane J AU - Krishnaswamy MR AU - Krzywdzinski S AU - Kubantsev M AU - Kuleshov S AU - Kulik Y AU - Kunori S AU - Landry F AU - Landsberg G AU - Leflat A AU - Li J AU - Li QZ AU - Lima JGR AU - Lincoln D AU - Linn SL AU - Linnemann J AU - Lipton R AU - Lu JG AU - Lucotte A AU - Lueking L AU - Maciel AKA AU - Madaras RJ AU - Magana-Mendoza L AU - Manankov V AU - Mani S AU - Mao HS AU - Markeloff R AU - Marshall T AU - Martin MI AU - Martin RD AU - Mauritz KM AU - May B AU - Mayorov AA AU - McCarthy R AU - McDonald J AU - McKibben T AU - McKinley J AU - McMahon T AU - Melanson HL AU - Merkin M AU - Merritt KW AU - Miao C AU - Miettinen H AU - Mincer A AU - Mishra CS AU - Mokhov N AU - Mondal NK AU - Montgomery HE AU - Mostafa M AU - da Motta H AU - Nang F AU - Narain P AU - Narasimham VS AU - Neal HA AU - Negret JP AU - Norman D AU - Oesch L AU - Oguri V AU - Oshima N AU - Owen D AU - Padley P AU - Para A AU - Parashar N AU - Park YM AU - Partridge R AU - Parua N AU - Paterno M AU - Patwa A AD - Univ Buenos Aires, Buenos Aires, DF, ArgentinaCtr Brasileiro Pesquisas Fis, LAFEX, Rio De Janeiro, BrazilUniv Estado Rio de Janeiro, Rio De Janeiro, BrazilInst High Energy Phys, Beijing 100039, Peoples R ChinaUniv Los Andes, Bogota, ColombiaUniv San Francisco Quito, Quito, EcuadorUniv Grenoble 1, IN2P3 CNRS, Inst Sci Nucl, Grenoble, FranceCtr Phys Particules Marseille, IN2P3 CNRS, Marseille, FranceCEA, DAPNIA Serv Phys Particules, Saclay, FrancePanjab Univ, Chandigarh 160014, IndiaUniv Delhi, Delhi 110007, IndiaTata Inst Fundamental Res, Mumbai, IndiaKyungsung Univ, Pusan 608736, South KoreaSeoul Natl Univ, Seoul, South KoreaCINVESTAV, Mexico City 14000, DF, MexicoInst Nucl Phys, Krakow, PolandInst Theoret & Expt Phys, Moscow 117259, RussiaMoscow State Univ, Moscow, RussiaInst High Energy Phys, Protvino, RussiaUniv Lancaster, Lancaster, EnglandUniv Arizona, Tucson, AZ 85721, USAUniv Calif Berkeley, Lawrence Berkeley Lab, Berkeley, CA 94720, USAUniv Calif Davis, Davis, CA 95616, USAUniv Calif Irvine, Irvine, CA 92697, USAUniv Calif Riverside, Riverside, CA 92521, USAFlorida State Univ, Tallahassee, FL 32306, USAUniv Hawaii, Honolulu, HI 96822, USAFermi Natl Accelerator Lab, Batavia, IL 60510, USAUniv Illinois, Chicago, IL 60607, USANo Illinois Univ, De Kalb, IL 60115, USANorthwestern Univ, Evanston, IL 60208, USAIndiana Univ, Bloomington, IN 47405, USAUniv Notre Dame, Notre Dame, IN 46556, USAPurdue Univ, W Lafayette, IN 47907, USAIowa State Univ, Ames, IA 50011, USAUniv Kansas, Lawrence, KS 66045, USAKansas State Univ, Manhattan, KS 66506, USALouisiana Tech Univ, Ruston, LA 71272, USAUniv Maryland, College Pk, MD 20742, USABoston Univ, Boston, MA 02215, USANortheastern Univ, Boston, MA 02115, USAUniv Michigan, Ann Arbor, MI 48109, USAMichigan State Univ, E Lansing, MI 48824, USAUniv Nebraska, Lincoln, NE 68588, USAColumbia Univ, New York, NY 10027, USANYU, New York, NY 10003, USAUniv Rochester, Rochester, NY 14627, USASUNY Stony Brook, Stony Brook, NY 11794, USABrookhaven Natl Lab, Upton, NY 11973, USALangston Univ, Langston, OK 73050, USAUniv Oklahoma, Norman, OK 73019, USABrown Univ, Providence, RI 02912, USAUniv Texas, Arlington, TX 76019, USATexas A&M Univ, College Stn, TX 77843, USARice Univ, Houston, TX 77005, USAUniv Washington, Seattle, WA 98195, USAAbbott, B, Univ Buenos Aires, Buenos Aires, DF, Argentina TI - Measurement of the W boson mass using electrons at large rapidities AB - We report a measurement of the W boson mass based on an integrated luminosity of 82 pb(-1) from
collisions at root s = 1.8 TeV recorded in 1994-1995 by the D0 detector at the Fermilab Tevatron. We identify W bosons by their decays to ev, where the electron is detected in the forward calorimeters. We extract the mass by fitting the transverse mass and the electron and neutrino transverse momentum spectra of 11 089 W boson candidates. We measure M-w = 80.691 +/- 0.227 GeV. By combining this measurement with our previously published central calorimeter results from data taken in 1992-1993 and 1994-1995, we obtain M-w = 80.482 +/- 0.091 GeV
MH - Argentina
MH - Brazil
MH - Colombia
MH - Ecuador
MH - United Kingdom
MH - France
MH - India
MH - Mexico|Distrito Federal
MH - Peoples R China
MH - Poland
MH - Russia
MH - South Korea
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 18
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0031-9007
UR - ISI:000084661500005
L2 - PARTON DISTRIBUTIONS; RADIATIVE-CORRECTIONS; FERMILAB-TEVATRON; GLOBAL ANALYSIS; D0 DETECTOR; COLLISIONS; COLLIDER; DECAY
SO - Physical Review Letters 2000 ;84(2):222-227
18
UI - 15730
AU - Aboytes F
AU - Sanchez F
AU - Cabra AIM
AU - Castro JEG
AD - Comis Fed Elect, Ctr Nacl Control Energia, Unidad Ingn Avanzada, Mexico City, DF, MexicoUniv Autonoma Nuevo Leon, Fac Ingn Mecan & Elect, Programa Doctoral Ingn Elect, Monterrey, NL, MexicoInterconex Elect SA, Medellin, ColombiaAboytes, F, Comis Fed Elect, Ctr Nacl Control Energia, Unidad Ingn Avanzada, Mexico City, DF, Mexico
TI - Dynamic stability analysis of the interconnected Colombia-Venezuela power system
AB - This paper presents the operating problems of the interconnection between Colombia and Venezuela power systems through a single 230 kV transmission line. It describes the technical analysis carried out for the stabilization of a sustained power flow oscillation of 0.22 Hz. The analysis includes results of simulations and field recordings obtained in the system. Operating strategies adopted and the conclusions of the study are also summarized
MH - Colombia
MH - Mexico|Distrito Federal
MH - Mexico|Nuevo Leon
PB - NEW YORK: IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
RP - NOT IN FILE
U3 - TC 0
U4 - Engineering, Electrical & Electronic
U5 - J;Article
AV - English
IS - 0885-8950
UR - ISI:000087916000055
L2 - excitation control;interarea oscillations;modal analysis;power system stabilizers;weak power systems
SO - Ieee Transactions on Power Systems 2000 ;15(1):376-381
19
UI - 16032
AU - Acevedo L
AU - Martinez E
AU - Castaneda P
AU - Franzblau S
AU - Timmermann BN
AU - Linares E
AU - Bye R
AU - Mata R
AD - Natl Autonomous Univ Mexico, Fac Quim, Dept Farmacia, Mexico City 04510, DF, MexicoGWL Hansens Dis Ctr, Baton Rouge, LA, USAUniv Arizona, Coll Pharm, Dept Pharmacol & Toxicol, Tucson, AZ 85721, USAUniv Nacl Autonoma Mexico, Inst Biol, Mexico City 04510, DF, MexicoMata, R, Natl Autonomous Univ Mexico, Fac Quim, Dept Farmacia, Mexico City 04510, DF, Mexico
TI - New phenylethanoids from Buddleja cordata subsp cordata
AB - Bioassay-guided fractionation of a crude extract of the stem bark of Buddleja cordata subsp. cordata with significant antimycobacterial activity led to the isolation of a mixture composed by ten new long-chain esters of 2[4'-hydroxyphenyl]-ethanol (1-10), along with the lichen metabolites methyl beta-orcinolcarboxylate (11) and beta-orcinolcarboxylate (12). Extensive HPLC allowed the separation of the major components of the mixture, which were characterized by spectral means as 2[4'-hydroxyphenyl]-ethyl stearate (3), 2[4'-hydroxyphenyl]-ethyl behenate (6), and 2[4'-hydroxyphenyl]-ethyl lignocerate (8). The minor esters were identified as 2[4'-hydroxyphenyl]-ethyl palmitate (1), 2[4'-hydroxyphenyl]-ethyl heptadecanoate (2), 2[4'-hydroxyphenyl]-ethyl nonadecanoate (4), 2[4'-hydroxyphenyl]-ethyl arachidate (5), 2[4'-hydroxyphenyl]-ethyl tricosanoate (7), 2[4'-hydroxyphenyl]-ethyl pentacosanoate (9), and 2[4'-hydroxyphenyl]-ethyl hexacosanoate (10) by GC-MS analysis of the methyl esters derivatives of the fatty acids obtained by alkaline hydrolysis of the mixture. Compound 8 exhibited moderate antibacterial activity against Mycobacterium tuberculosis (MIC = 64 mu g/ml)
MH - Mexico|Distrito Federal
MH - USA
PB - STUTTGART: GEORG THIEME VERLAG
RP - NOT IN FILE
U3 - TC 2
U4 - Plant Sciences;Chemistry, Medicinal;Pharmacology & Pharmacy
U5 - J;Article
AV - English
IS - 0032-0943
UR - ISI:000086893900012
L2 - Buddleja cordata subsp cordata;Loganiaceae;phenylethanoids;Mycobacterium tuberculosis;antimycobacterial activity;methyl beta-orcinolcarboxylate;beta-orcinolcarboxylate;LINARIN
SO - Planta Medica 2000 ;66(3):257-261
20
UI - 15227
AU - Aceves SM
AU - Martinez-Frias J
AU - Garcia-Villazana O
AD - Univ Calif Lawrence Livermore Natl Lab, Livermore, CA 94551, USACtr Ingn & Desarrollo Ind, Queretaro, Qro, MexicoUniv Guanajuato, FIMEE, Salamanca, Gto, MexicoAceves, SM, Univ Calif Lawrence Livermore Natl Lab, 7000 East Ave,L-641, Livermore, CA 94551 USA
TI - Analytical and experimental evaluation of insulated pressure vessels for cryogenic hydrogen storage
AB - Insulated pressure vessels are cryogenic-capable pressure vessels that can be fueled with liquid hydrogen (LH2) or ambient-temperature compressed hydrogen (CH2). These vessels offer the advantages of LH2 tanks (low weight and volume), with reduced disadvantages (fuel flexibility, lower energy requirement for hydrogen liquefaction and reduced evaporative losses). The work described here is directed to verify that commercially available pressure vessels can be safely used to store LH2. The use of commercially available pressure vessels significantly reduces the cost and complexity of the insulated pressure vessel development effort. This paper describes a series of tests that have been done with aluminum-lined, fiber-wrapped vessels to evaluate the damage caused by low temperature operation. All analyses and experiments to date indicate that no significant damage has resulted. Required future tests are described, which will prove that no technical barriers exist to the safe use of aluminum-fiber vessels at cryogenic temperatures. Published by Elsevier Science Ltd on behalf of the International Association for Hydrogen Energy
MH - USA
MH - Mexico|Guanajuato
MH - Mexico|Queretaro
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 6
U4 - Chemistry, Physical;Energy & Fuels;Environmental Sciences;Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 0360-3199
UR - ISI:000089397900008
SO - International Journal of Hydrogen Energy 2000 ;25(11):1075-1085
21
UI - 15729
AU - Acha E
AU - mbriz-Perez H
AU - Fuerte-Esquivel CR
AD - Univ Glasgow, Virtual FACTS Res Lab, Dept Elect & Elect Engn, Glasgow G12 8QQ, Lanark, ScotlandInst Technol, Dept Ingn Elect & Elect, Virtual FACTS Res Lab, Morelia, Michoacan, MexicoAcha, E, Univ Glasgow, Virtual FACTS Res Lab, Dept Elect & Elect Engn, Glasgow G12 8QQ, Lanark, Scotland
TI - Advanced transformer control modeling in an optimal power flow using Newton's method
AB - This paper reports on advanced transformer modeling facilities suitable for large-scale optimal power flow studies. The new transformer models are developed from first principles and incorporated into an existing Newton-based optimal power flow computer program for highly robust iterative solutions. A three-winding transformer model with tap ratios in all three windings is shown to be a general case for existing two-winding transformer models and the classic load tap-changing and phase-shifting transformer models. The newly developed transformer models add a great deal to software flexibility and are amenable to more realistic electric energy studies. This is partly due to the transformer models being fitted with complex tap changers in each winding and a nonlinear representation of the magnetizing branch. The three-winding transformer model interfaces easily with reactive power plant models, e.g., static var compensators
MH - Mexico|Michoacan
MH - United Kingdom
PB - NEW YORK: IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
RP - NOT IN FILE
U3 - TC 1
U4 - Engineering, Electrical & Electronic
U5 - J;Article
AV - English
IS - 0885-8950
UR - ISI:000087916000043
L2 - FACTS;load tap-changing transformers;Newton's method;optimal power flows;phase-shifting transformers;ALGORITHM; NETWORKS
SO - Ieee Transactions on Power Systems 2000 ;15(1):290-298
22
UI - 14675
AU - Acosta CR
AU - Acosta M
AU - Sosa V
AU - Ares O
AD - IPN, CINVESTAV, Unidad Merida, Dept Fis Aplicada, Merida 97310, Yucatan, MexicoUH, Fac Fis, IMRE, Lab Superconduct, La Habana 10400, CubaAcosta, CR, IPN, CINVESTAV, Unidad Merida, Dept Fis Aplicada, AP 73 Cordemex, Merida 97310, Yucatan, Mexico
TI - Comparative analysis of the determination of J(c) of YBCO films at different temperatures and magnetic fields by means of the shielding technique
AB - Imaginary susceptibility of YBCO films was studied between 32 and 83 K as a function of magnetic field (0 to 350 Oe). No maximum in the curve of susceptibility was observed at low temperatures ((i)50 K), this made that this criterion for the determination of the critical current density could not be applied. The same fact ocurred in the curves of the third harmonic against magnetic field. Therefore, to determine J(c) we proposed the criterion of taking the maximum of the third/first harmonic ratio. It was observed that the J(c) values determined with the three criteria tend to coincide as they approach to the critical temperature
MH - Cuba
MH - Mexico|Yucatan
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 1
U4 - Physics, Applied
U5 - J;Article
AV - English
IS - 0921-4534
UR - ISI:000165855900252
L2 - AC SUSCEPTIBILITY MEASUREMENTS; SUPERCONDUCTORS
SO - Physica C 2000 ;341():2051-2052
23
UI - 16437
AU - Acosta CR
AU - Acosta M
AU - Sosa V
AU - Ares O
AD - IPN, CINVESTAV, Dept Fis Aplicada, Unidad Merida, Merida 97310, Yucatan, MexicoUH Fac Fis, Lab Superconduct IMRE, La Habana 10400, CubaAcosta, CR, IPN, CINVESTAV, Dept Fis Aplicada, Unidad Merida, AP 73 Cordemex, Merida 97310, Yucatan, Mexico
TI - Screening technique measurement of ac imaginary susceptibility and critical current density of YBa2Cu3O7-delta films
AB - The screening technique was used to study systematically the ac susceptibility of superconducting YBa2Cu3O7-delta thin films in the temperature range of 32-83 K. We used the Fourier transform of the pick-up signal, coming from the secondary coil, to estimate the critical current density. From the experimental data we observed regularities in the imaginary part of ac susceptibility, and confirmed that the flux creep mechanism is dominant. (C) 2000 American Institute of Physics. [S0021-8979(00)03105-4]
MH - Cuba
MH - Mexico|Yucatan
PB - MELVILLE: AMER INST PHYSICS
RP - NOT IN FILE
U3 - TC 1
U4 - Physics, Applied
U5 - J;Article
AV - English
IS - 0021-8979
UR - ISI:000085529500064
L2 - HIGH-TEMPERATURE SUPERCONDUCTORS; MAGNETIC-FIELD; THIN-FILMS; DISKS; TC
SO - Journal of Applied Physics 2000 ;87(5):2460-2463
24
UI - 14955
AU - Acosta DR
AU - Estrada W
AU - Castanedo R
AU - Maldonado A
AU - Valenzuela MA
AD - Univ Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoUNI, Fac Ciencias, Lima, PeruCINVESTAV, IPN, Mat Lab, Queretaro, MexicoCINVESTAV, IPN, Mexico City 07000, DF, MexicoESIQUIE, IPN, Lab Catalisis & Mat, Mexico City 07738, DF, MexicoAcosta, DR, Univ Nacl Autonoma Mexico, Inst Fis, Apartado Postal 20364, Mexico City 01000, DF, Mexico
TI - Structural and surface studies of tin oxide films doped with fluorine
AB - Thin films of SnO2:F deposited by spray pyrolysis over glass substrate at 300 degreesC, were studied by scanning, conventional and high resolution electron microscopy together with atomic force microscopy. The surface topology and morphology changes detected for films deposited with various fluorine levels are related to the electrical behavior previously reported. (C) 2000 Elsevier Science S.A. All rights reserved
MH - Mexico|Distrito Federal
MH - Mexico|Queretaro
MH - Peru
PB - LAUSANNE: ELSEVIER SCIENCE SA
RP - NOT IN FILE
U3 - TC 0
U4 - Materials Science, Multidisciplinary;Materials Science, Coatings & Films;Physics, Applied;Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0040-6090
UR - ISI:000165067400033
L2 - thin films;SnO2;fluorine doping;electron microscopy;atomic force microscopy
SO - Thin Solid Films 2000 ;375(1-2):147-150
25
UI - 16461
AU - Acosta LR
AU - Evans WFJ
AD - SIMA, Mexico City 06900, DF, MexicoTrent Univ, Atmospher Phys Lab, Environm Resource Studies, Peterborough, ON K9J 7B8, CanadaAcosta, LR, SIMA, Apto Post 71-70, Mexico City 06900, DF, Mexico
TI - Design of the Mexico City UV monitoring network: UV-B measurements at ground level in the urban environment
AB - Although there is concern for future stratospheric ozone depletion, several large urban populations are already being exposed to very high UV levels due to geographical factors. In Mexico City, ultraviolet radiation (UV) plays an important role in the generation of high levels of tropospheric ozone and other photochemical pollutants. The measurement of ultraviolet-B radiation in Mexico began in the spring 1993, as a pilot project for ultraviolet-B (UV-B) monitoring and as support for the first Hispanic public information program on the UV index through the Televisa (Mexican television network, which covers the Spanish speaking world). In 1996, based on our preliminary measurements, the Mexico City government commissioned the authors to design the Valley of Mexico UV-monitoring Network. The design of the network is presented. The preliminary measurements show that biologically active (UV-B) solar radiation can reach levels above 5 minimum erythemal dose (MED/hour) or 12 UV index units during spring and summer months. Annual UV measurements have shown seasonal variations of 40% between winter and summer months. Strong attenuation of UV-B radiation at ground level in the urban triosphere has been detected under polluted conditions. Measurements of the morphology of UV-B radiation have been taken at downtown and suburban monitoring stations, over diurnal, monthly and yearly periods. The network measurements show that the downtown UV-B levels are 20% lower than suburban levels on a seasonal basis, but differences can be greater than 40% on polluted days. The relationship between the Total Ozone Mapping Spectrometer (TOMS) total ozone column and tropospheric ozone concentrations in Mexico City is also discussed
MH - Canada
MH - Mexico|Distrito Federal
PB - WASHINGTON: AMER GEOPHYSICAL UNION
RP - NOT IN FILE
U3 - TC 10
U4 - Meteorology & Atmospheric Sciences
U5 - J;Article
AV - English
IS - 0747-7309
UR - ISI:000085512800061
L2 - OZONE; ULTRAVIOLET
SO - Journal of Geophysical Research-Atmospheres 2000 ;105(D4):5017-5026
26
UI - 14668
AU - Adhikari SK
AU - Casas M
AU - Puente A
AU - Rigo A
AU - Fortes M
AU - Solis MA
AU - de Llano M
AU - Valladares AA
AU - Rojo O
AD - Univ Estadual Paulista, Inst Fis Teor, BR-01405900 Sao Paulo, BrazilUniv Illes Balears, Dept Fis, Palma de Mallorca 07071, SpainUniv Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoUniv Nacl Autonoma Mexico, Inst Invest Mat, Mexico City 04510, DF, MexicoPESTIC, Secretaria Acad, Mexico City 04430, DF, MexicoCINVESTAV, IPN, Mexico City 04430, DF, MexicoAdhikari, SK, Univ Estadual Paulista, Inst Fis Teor, BR-01405900 Sao Paulo, Brazil
TI - Cooper pair dispersion relation in two dimensions
AB - The Cooper pair binding energy vs. center-of-mass-momentum dispersion relation for Bose-Einstein condensation studies of superconductivity is found in two dimensions for a renormalized attractive delta interaction. It crosses over smoothly from a linear to a quadratic form as coupling varies from weak to strong
MH - Brazil
MH - Mexico|Distrito Federal
MH - Spain
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 1
U4 - Physics, Applied
U5 - J;Article
AV - English
IS - 0921-4534
UR - ISI:000165855500039
L2 - BOSE-EINSTEIN CONDENSATION; SUPERCONDUCTIVITY; MODEL
SO - Physica C 2000 ;341():151-152
27
UI - 14670
AU - Adhikari SK
AU - Casas M
AU - Puente A
AU - Rigo A
AU - Fortes M
AU - Solis MA
AU - de Llano M
AU - Valladares AA
AU - Rojo O
AD - Univ Estadual Paulista, Inst Fis Teor, BR-01405900 Sao Paulo, BrazilUniv Illes Balears, Dept Fis, E-07071 Palma de Mallorca, SpainUniv Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoNatl Autonomous Univ Mexico, Inst Invest Mat, Mexico City 04510, DF, MexicoPESTIC, Secretaria Acad, Mexico City 04430, DF, MexicoIPN, CINVESTAV, Mexico City 04430, DF, MexicoAdhikari, SK, Univ Estadual Paulista, Inst Fis Teor, Rua Pamplona 145, BR-01405900 Sao Paulo, Brazil
TI - Superconductivity as a Bose-Einstein condensation?
AB - Bose-Einstein condensation (BEC) in two dimensions (2D) (e.g., to describe the quasi-2D cuprates) is suggested as the possible mechanism widely believed to underlie superconductivity in general. A crucial role is played by nonzero center-of-mass momentum Cooper pairs (CPs) usually neglected in BCS theory. Also vital is the unique linear dispersion relation appropriate to weakly-coupled "bosonic" CPs moving in the Fermi sea-rather than in vacuum where the dispersion would be quadratic but only for very strong coupling, and for which BEC is known to be impossible in 2D
MH - Brazil
MH - Mexico|Distrito Federal
MH - Spain
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 0
U4 - Physics, Applied
U5 - J;Article
AV - English
IS - 0921-4534
UR - ISI:000165855500074
L2 - ORGANIC SUPERCONDUCTORS; PENETRATION-DEPTH
SO - Physica C 2000 ;341():233-236
28
UI - 15070
AU - Adhikari SK
AU - Casas M
AU - Puente A
AU - Rigo A
AU - Fortes M
AU - Solis MA
AU - de Llano M
AU - Valladares AA
AU - Rojo O
AD - Univ Estadual Paulista, Inst Fis Teor, BR-01405900 Sao Paulo, BrazilUniv Illes Balears, Dept Fis, E-07071 Palma de Mallorca, SpainUniv Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoNatl Autonomous Univ Mexico, Inst Invest Mat, Mexico City 04510, DF, MexicoSecretaria Acad, PESTIC, Mexico City 04430, DF, MexicoIPN, CINVESTAV, Mexico City 04430, DF, MexicoAdhikari, SK, Univ Estadual Paulista, Inst Fis Teor, BR-01405900 Sao Paulo, Brazil
TI - Cooper pair dispersion relation for weak to strong coupling
AB - Cooper pairing in two dimensions is analyzed with a set of renormalized equations to determine its binding energy for any fermion number density and all coupling assuming a,generic pairwise residual interfermion interaction. Also considered are Cooper pairs (CP's) with nonzero center-of-mass momentum (CMM) and their binding energy is expanded analytically in powers of the CMM up to quadratic terms. A Fermi-sea-dependent linear term in the CMM dominates the pair excitation energy in weak coupling (also called the BCS regime) while the more familiar quadratic term prevails in strong coupling (the Bose regime). The crossover, though strictly unrelated to BCS theory per se, is studied numerically as it is expected to play a central role in a model of superconductivity as a Bose-Einstein condensation of CPs where the transition temperature vanishes for all dimensionality d less than or equal to 2 for quadratic dispersion, but is nonzero for all d greater than or equal to 1 for linear dispersion
MH - Brazil
MH - Mexico|Distrito Federal
MH - Spain
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 18
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0163-1829
UR - ISI:000089733800030
L2 - BOSE CONDENSATION; BCS; SUPERCONDUCTIVITY; MODEL; RENORMALIZATION; CROSSOVER; WAVES; GAS
SO - Physical Review B 2000 ;62(13):8671-8674
29
UI - 14521
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Beier C
AU - Belousov A
AU - Benisch T
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bertrand-Coremans G
AU - Bizot JC
AU - Borras K
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Broker HB
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Bunyatyan A
AU - Burkhardt H
AU - Burrage A
AU - Buschhorn G
AU - Campbell AJ
AU - Cao J
AU - Carli T
AU - Caron S
AU - Chabert E
AU - Clarke D
AU - Clerbaux B
AU - Collard C
AU - Contreras JG
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - Delcourt B
AU - Delerue N
AU - Demirchyan R
AU - De Roeck A
AU - De Wolf EA
AU - Diaconu C
AU - Dixon P
AU - Dodonov V
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Duprel C
AU - Ebert J
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Ellerbrock M
AU - Elsen E
AU - Erdmann M
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Ferencei J
AU - Ferrarotto F
AU - Ferron S
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Foresti I
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Goodwin C
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Haustein V
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herrera G
AU - Herynek I
AU - Hilgers M
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoting P
AU - Hoffmann D
AU - Hoprich W
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Janssen X
AU - Jemanov V
AU - Jonsson L
AU - Johnson DP
AU - Jones MAS
AU - Jung H
AU - Kastli HK
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnick O
AU - Kaufmann O
AU - Kausch M
AU - Keil F
AU - Keller N
AU - Kennedy J
AU - Kenyon IR
AU - Kermiche S
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Koblitz B
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Krasny MW
AU - Krehbiel H
AU - Kroseberg J
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuhr T
AU - Kurca T
AU - Kutuev R
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Lastovicka T
AU - Lebedev A
AU - Leissner B
AU - Lemaitre V
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobo G
AU - Lobodzinska E
AU - Lobodzinski B
AU - Loktionova N
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mkrtchyan T
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon MN
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller D
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Nellen G
AU - Newman PR
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Olsson JE
AU - Ozerov D
AU - Panassik V
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Perez E
AU - Phillips JP
AU - Pitzl D
AU - Poschl R
AU - Potachnikova I
AU - Povh B
AU - Rabbertz K
AU - Radel G
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham, W Midlands, EnglandInteruniv Inst High Energies, ULB, VUB, Brussels, BelgiumUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Nucl Phys, Krakow, PolandUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Inst Nucl Res, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Kirchhoff Inst Phys, Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Mat, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Mediterranne, IN2P3, CNRS, CPPM, Marseille, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, IN2P3, CNRS, LAL, Orsay, FranceEcole Polytech, LPNHE, IN2P3, CNRS, Palaiseau, FranceUniv Paris 06, LPNHE, Paris, FranceUniv Paris 07, IN2P3, CNRS, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Fac Math & Phys, Prague, Czech RepublicIst Nazl Fis Nucl, Rome, ItalyUniv Roma 3, Dipartimento Fis, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandYerevan Phys Inst, Zeuthen, GermanyDESY, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandBerg Univ Gesamthsch Wuppertal, Rechtzentrum, Wuppertal, GermanyUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Ap, Merida, Yucatan, MexicoSafarik Univ, Kosice, SlovakiaCERN, Geneva, SwitzerlandAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - Inclusive photoproduction of neutral pions in the photon hemisphere at HERA
AB - The inclusive cross section for the photoproduction of neutral pious has been measured as a function of the transverse momentum, rapidity, and Feynman x of the pi (0) mesons at an average photon-proton centre-of-mass energy of 208 GeV and for photon virtualities below Q(2) = 0.01 GeV2. The pi (0) measurement extends the range covered by previous charged particle measurements at HERA by two units of rapidity in the photon direction down to a value of -5.5 in the gammap centre-of-mass frame. The pi (0) transverse momentum distribution is well described over the whole measured range by a power law ansatz, while an exponential fit falls below the data at transverse momentum values above 1.5 GeV/c. Good agreement with the predictions of the Monte Carlo models PYTHIA and PHOJET is found. In the context of the PYTHIA model the data are inconsistent with large intrinsic transverse momentum values in the photon
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
PB - NEW YORK: SPRINGER-VERLAG
RP - NOT IN FILE
U3 - TC 1
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000166416700006
L2 - LARGE TRANSVERSE-MOMENTUM; LIQUID ARGON CALORIMETER; LEAD/SCINTILLATING-FIBER CALORIMETER; HIGH-ENERGY PHOTOPRODUCTION; PARTICLE CROSS-SECTIONS; LUND MONTE-CARLO; PARTON FRAGMENTATION; PP INTERACTIONS; H1 DETECTOR; PI-0 MESONS
SO - European Physical Journal C 2000 ;18(2):293-302
30
UI - 14739
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Beier C
AU - Belousov A
AU - Benisch T
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bizot JC
AU - Borras K
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Broker HB
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Bunyatyan A
AU - Burkhardt H
AU - Burrage A
AU - Buschhorn G
AU - Campbell AJ
AU - Cao J
AU - Carli T
AU - Caron S
AU - Chabert E
AU - Clarke D
AU - Clerbaux B
AU - Collard C
AU - Contreras JG
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - Davidsson M
AU - Delcourt B
AU - Delerue N
AU - Demirchyan R
AU - De Roeck A
AU - De Wolf EA
AU - Diaconu C
AU - Dixon P
AU - Dodonov V
AU - Dowell JD
AU - Droutskoi A
AU - Duprel C
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Ellerbrock M
AU - Elsen E
AU - Erdmann M
AU - Erdmann W
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Ferencei J
AU - Ferron S
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Foresti I
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Goodwin C
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herrera G
AU - Herynek I
AU - Hilgers M
AU - Hiller KH
AU - Hladky J
AU - Hoting P
AU - Hoffmann D
AU - Hoprich W
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Janssen X
AU - Jemanov V
AU - Jonsson L
AU - Johnson DP
AU - Jones MAS
AU - Jung H
AU - Kastli HK
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnick O
AU - Kaufmann O
AU - Kausch M
AU - Keil F
AU - Keller N
AU - Kennedy J
AU - Kenyon IR
AU - Kermiche S
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Koblitz B
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Krasny MW
AU - Krehbiel H
AU - Kroseberg J
AU - Kruger K
AU - Kupper A
AU - Kuhr T
AU - Kurca T
AU - Kutuev R
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Lastovicka T
AU - Lebailly E
AU - Lebedev A
AU - Leissner B
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobodzinska E
AU - Lobodzinski B
AU - Loktionova N
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mkrtchyan T
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon MN
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Nellen G
AU - Newman PR
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Olsson JE
AU - Ozerov D
AU - Panassik V
AU - Pascaud C
AU - Patel GD
AU - Perez E
AU - Phillips JP
AU - Pitzl D
AU - Poschl R
AU - Potachnikova I
AU - Povh B
AU - Rabbertz K
AU - Radel G
AU - Rauschenberger J
AU - Reimer P
AU - Reisert B
AU - Reyna D
AU - Riess S
AU - Rizvi E
AU - Robmann P
AU - Roosen R
AU - Rostovtsev A
AU - Royon C
AU - Rusakov S
AU - Rybicki K
AU - Sankey DPC
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandUniv Instelling Antwerp, Wilrijk, BelgiumFree Univ Brussels, Interuniv Inst High Energies, Brussels, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Nucl Phys, Krakow, PolandUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Inst Nucl Res, Dubna, RussiaCEA Saclay, DSM, DAPNIA, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Kirchhoff Inst Phys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Mediterranee, CPPM, CNRS, IN2P3, Marseille, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, LAL, IN2P3, CNRS, Orsay, FranceEcole Polytech, LPNHE, IN2P3, CNRS, Palaiseau, FranceUniv Paris 06, LPNHE, Paris, FranceUniv Paris 07, IN2P3, CNRS, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Fac Math & Phys, Prague, Czech RepublicUniv Roma 3, Ist Nazl Fis Nucl, Rome, ItalyUniv Roma 3, Dipartimento Fis, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandBerg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyYerevan Phys Inst, Yerevan 375036, ArmeniaDESY, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyAp CINVESTAV, Dept Fis, Yucatan, MexicoSafarik Univ, Kosice, SlovakiaCERN, Geneva, SwitzerlandAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - A search for excited fermions at HERA
AB - A search for excited fermions f* of the first generation in e(+)p scattering at the collider HERA is presented using H1 data with an integrated luminosity of 37 pb(-1). All electroweak decays of excited fermions, f* --> f gamma fW, fZ are considered and all possible final states resulting from the Z or W hadronic decays or decays into leptons of the first two generations are taken into account. No evidence for f* production is found. Mass dependent exclusion limits on cross-sections and on the ratio of coupling constants to the compositeness scale are derived
MH - Armenia
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
PB - NEW YORK: SPRINGER-VERLAG
RP - NOT IN FILE
U3 - TC 18
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000165688600002
L2 - LIQUID ARGON CALORIMETER; DYNAMICAL SYMMETRY BREAKING; ENERGY EP COLLISIONS; LEPTON PRODUCTION; H1; SUBSTRUCTURE; SCATTERING; COLLIDERS; QUARKS; CALIBRATION
SO - European Physical Journal C 2000 ;17(4):567-581
31
UI - 15735
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Behnke O
AU - Beier C
AU - Belousov A
AU - Benisch T
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bertrand-Coremans G
AU - Biddulph P
AU - Bizot JC
AU - Borras K
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Broker HB
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Bunyatyan A
AU - Burke S
AU - Burkhardt H
AU - Burrage A
AU - Buschhorn G
AU - Campbell AJ
AU - Cao J
AU - Carli T
AU - Chabert E
AU - Charlet M
AU - Clarke D
AU - Clerbaux B
AU - Collard C
AU - Contreras JG
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - Delcourt B
AU - De Roeck A
AU - De Wolf EA
AU - Diaconu C
AU - Dixon P
AU - Dodonov V
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Duprel C
AU - Ebert J
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Ellerbrock M
AU - Elsen E
AU - Erdmann M
AU - Fahr AB
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Feltesse J
AU - Ferencei J
AU - Ferrarotto F
AU - Ferron S
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Foresti I
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Gorelov I
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Griffiths RK
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Haustein V
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herrera G
AU - Herynek I
AU - Hilgers M
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoting P
AU - Hoffmann D
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Janssen X
AU - Jonsson L
AU - Johnson DP
AU - Jones M
AU - Jung H
AU - Kastli HK
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnick O
AU - Kaufmann O
AU - Kausch M
AU - Keil F
AU - Keller N
AU - Kenyon IR
AU - Kermiche S
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Krasny MW
AU - Krehbiel H
AU - Kroseberg J
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuhr T
AU - Kurca T
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Lebedev A
AU - Lehner F
AU - Lemaitre V
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobo G
AU - Lobodzinska E
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - McMahon TR
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon MN
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller D
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Newman PR
AU - Nguyen HK
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Olsson JE
AU - Ozerov D
AU - Panassik V
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Perez E
AU - Phillips JP
AU - Pitzl D
AU - Poschl R
AU - Potashnikova I
AU - Povh B
AU - Rabbertz K
AU - Radel G
AU - Rauschenberger J
AU - Reimer P
AU - Reisert B
AU - Reyna D
AU - Riess S
AU - Rizvi E
AU - Robmann P
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, D-42097 Wuppertal, GermanyRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 2, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandVUB, ULB, Inter Univ Inst High Energies, Brussels, BelgiumUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Nucl Phys, Krakow, PolandUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Inst Nucl Res, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Inst Hochenergiephys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Aix Marseille 2, CNRS, IN2P3, CPPM, F-13284 Marseille 07, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris 11, CNRS, IN2P3, LAL, Orsay, FranceEcole Polytech, CNRS, IN2P3, LPHNE, F-91128 Palaiseau, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Nucl Ctr, Prague, Czech RepublicIst Nazl Fis Nucl Roma 1, Rome, ItalyUniv Roma 3, Dipartimento Fis, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandBerg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyYerevan Phys Inst, Yerevan 375036, ArmeniaDESY, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandBerg Univ Gesamthsch Wuppertal, Rechenzentrum, Wuppertal, GermanyUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Ap, Merida, Yucatan, MexicoSafarik Univ, SK-04154 Kosice, SlovakiaAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, D-42097 Wuppertal, Germany
TI - Investigation of power corrections to event shape variables measured in deep-inelastic scattering
AB - Deep-inelastic ep scattering data, taken with the H1 detector at HERA, are used to study the event shape variables thrust, jet broadening, jet mass, C parameter and two kinds of differential two-jet rate. The data cover a large range of the four-momentum transfer Q, which is considered to be the relevant energy scale, between 7GeV and 100 GeV. The Q dependences of the mean values are compared with second order calculations of perturbative QCD applying power law corrections proportional to 1/Q(p) to account for hadronization effects. The concept of power corrections is investigated by fitting simultaneously a non-perturbative parameter <(alpha)over bar>(p-1) and the strong coupling constant a,
MH - Armenia
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 22
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000087883300005
L2 - MONTE-CARLO GENERATOR; PARTON DISTRIBUTIONS; JET FRAGMENTATION; E+E ANNIHILATION; PETRA ENERGIES; CROSS-SECTIONS; QCD; PHYSICS; HERA; DEPENDENCE
SO - European Physical Journal C 2000 ;14(2):255-269
32
UI - 15753
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Beier C
AU - Belousov A
AU - Benisch T
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bizot JC
AU - Borras K
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Broker HB
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Bunyatyan A
AU - Burkhardt H
AU - Burrage A
AU - Buschhorn G
AU - Campbell AJ
AU - Cao J
AU - Carli T
AU - Caron S
AU - Chabert E
AU - Clarke D
AU - Clerbaux B
AU - Collard C
AU - Contreras JG
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - Delcourt B
AU - Delerue N
AU - Demirchyan R
AU - De Roeck A
AU - De Wolf EA
AU - Diaconu C
AU - Dixon P
AU - Dodonov V
AU - Dowell JD
AU - Droutskoi A
AU - Duprel C
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Ellerbrock M
AU - Elsen E
AU - Erdmann M
AU - Erdmann W
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Ferencei J
AU - Ferron S
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Foresti I
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Goodwin C
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herrera G
AU - Herynek I
AU - Hilgers M
AU - Hiller KH
AU - Hladky J
AU - Hoting P
AU - Hoffmann D
AU - Hoprich W
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Janssen X
AU - Jemanov V
AU - Jonsson L
AU - Johnson DP
AU - Jones MAS
AU - Jung H
AU - Kastli HK
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnick O
AU - Kaufmann O
AU - Kausch M
AU - Keil F
AU - Keller N
AU - Kennedy J
AU - Kenyon IR
AU - Kermiche S
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Koblitz B
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Krasny MW
AU - Krehbiel H
AU - Kroseberg J
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuhr T
AU - Kurca T
AU - Kutuev R
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Lastovicka T
AU - Lebedev A
AU - Leissner B
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobodzinska E
AU - Lobodzinski B
AU - Loktionova N
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mkrtchyan T
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon MN
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Nellen G
AU - Newman PR
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Olsson JE
AU - Ozerov D
AU - Panassik V
AU - Pascaud C
AU - Patel GD
AU - Perez E
AU - Phillips JP
AU - Pitzl D
AU - Poschl R
AU - Potachnikova I
AU - Povh B
AU - Rabbertz K
AU - Radel G
AU - Rauschenberger J
AU - Reimer P
AU - Reisert B
AU - Reyna D
AU - Riess S
AU - Rizvi E
AU - Robmann P
AU - Roosen R
AU - Rostovtsev A
AU - Royon C
AU - Rusakov S
AU - Rybicki K
AU - Sankey DPC
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 2, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandULB, VUB, Inter Univ Inst High Energies, Brussels, BelgiumUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Nucl Phys, Krakow, PolandUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Nucl Res Inst, Dubna 141980, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Kirchhoff Inst Phys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Mediterranee, CNRS, IN2P3, CPPM, Marseille, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris 11, CNRS, IN2P3, LAL, F-91405 Orsay, FranceEcole Polytech, CNRS, IN2P3, LPNHE, F-91128 Palaiseau, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Fac Math & Phys, Prague, Czech RepublicUniv Roma 3, INFN Roma 1, Rome, ItalyUniv Roma 3, Dipartimento Fis, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandYerevan Phys Inst, Yerevan 375036, ArmeniaDESY, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandHumboldt Univ, Inst Phys, Berlin, GermanyCINVESTAV, Dept Fis Ap, Merida, Yucatan, MexicoBerg Univ Gesamthsch Wuppertal, Rech Zentrum, Wuppertal, GermanyCERN, Geneva, SwitzerlandUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanySafarik Univ, Kosice, SlovakiaAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - Measurement of elastic electroproduction of phi mesons at HERA
AB - The elastic electroproduction of phi mesons is studied at HERA with the H1 detector for photon virtualities 1 < Q(2) < 15 GeV2 and hadronic centre of mass energies 40 < W < 130 GeV. The Q(2) and t dependences of the cross section are extracted (t being the square of the four-momentum transfer to the target proton). When plotted as function of (Q(2) + M-v(2)) and scaled by the appropriate SU(5) quark charge factor, the phi meson cross section agrees within errors with the cross sections of the vector mesons V = rho, omega and J/psi. A detailed analysis is performed of the phi meson polarisation state and the ratio of the production cross sections for longitudinally and transversely polarised phi mesons is determined. A small but significant violation of s-channel helicity conservation (SCKC) is observed. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Armenia
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 37
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0370-2693
UR - ISI:000087791700003
L2 - DEEP-INELASTIC SCATTERING; VECTOR-MESONS; DIFFRACTIVE ELECTROPRODUCTION; PHOTOPRODUCTION; RHO(0)
SO - Physics Letters B 2000 ;483(4):360-372
33
UI - 16015
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Behrend HJ
AU - Beier C
AU - Belousov A
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bertrand-Coremans G
AU - Biddulph P
AU - Bizot JC
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Broker HB
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Bunyatyan A
AU - Burke S
AU - Burrage A
AU - Buschhorn G
AU - Calvet D
AU - Campbell AJ
AU - Carli T
AU - Chabert E
AU - Charlet M
AU - Clarke D
AU - Clerbaux B
AU - Contreras JG
AU - Cormack C
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - De Roeck A
AU - De Wolf EA
AU - Delcourt B
AU - Demirchyan R
AU - Diaconu C
AU - Dirkmann M
AU - Dixon P
AU - Dodonov V
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Ebert J
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Elsen E
AU - Enzenberger M
AU - Erdmann M
AU - Fahr AB
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Feltesse J
AU - Ferencei J
AU - Ferrarotto F
AU - Ferron S
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Gaede F
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Gorelov I
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Griffiths RK
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Hampel M
AU - Haustein V
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herrera G
AU - Herynek I
AU - Hewitt K
AU - Hilgers M
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoting P
AU - Hoffmann D
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Jonsson L
AU - Johnson DP
AU - Jones M
AU - Jung H
AU - Kastli HK
AU - Kander M
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnick O
AU - Kaufmann O
AU - Kausch M
AU - Keil F
AU - Keller N
AU - Kenyon IR
AU - Kermiche S
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Kohne JH
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Kramerkamper T
AU - Krasny MW
AU - Krehbiel H
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuster H
AU - Kuhlen M
AU - Kurca T
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Langenegger U
AU - Lebedev A
AU - Lehner F
AU - Lemaitre V
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobo G
AU - Lobodzinska E
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - McMahon TR
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon MN
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller D
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Newman PR
AU - Nguyen HK
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Niedzballa C
AU - Niggli H
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Oberlack H
AU - Olsson JE
AU - Ozerov D
AU - Palmen P
AU - Panassik V
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Pawletta H
AU - Perez E
AU - Phillips JP
AU - Pieuchot A
AU - Pitzl D
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumFree Univ Brussels, Interuniv Inst High Energies, Brussels, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Phys Nucl, Krakow, PolandUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Nucl Res Inst, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, Heidelberg, Vic, AustraliaUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Inst Hochenergiephys, Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Aix Marseille 2, CPPM, IN2P3, CNRS, Marseille, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, LAL, IN2P3, CNRS, Orsay, FranceEcole Polytech, LPNHE, IN2P3, CNRS, Palaiseau, FranceUniv Paris 06, LPNHE, IN2P3, CNRS, Paris, FranceUniv Paris 07, LPNHE, IN2P3, CNRS, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Nucl Ctr, Prague, Czech RepublicUniv Roma 3, Ist Nazl Fis Nucl, Rome, ItalyUniv Roma 3, Dipartimento Fis, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandDESY, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandBerg Univ Gesamthsch Wuppertal, Rechenzentrum, Wuppertal, GermanyUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Aplicada, Merida, Yucatau, MexicoUniv PJ Safarik, Kosice, SlovakiaAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - Measurement of neutral and charged current cross-sections in positron-proton collisions at large momentum transfer
AB - The inclusive single and double differential cross-sections for neutral and charged charged processes with four-momentum transfer squared Q(2) between 150 and 30 000 GeV2 and with Bjorken x between 0.0032 and 0.65 are measured in e(+)p collisions. The data were taken with the H1 detector at HERA between 1994 and 1997. and they correspond to an integrated luminosity of 35.6 pb(-1). Tho Q(2) evolution of the parton densities of the proton is tested, yielding no significant deviation from the prediction of perturbative QCD. The proton structure function Fz(x, Q(2)) is determined. All extraction of the u and d quark distributions at high x is presented. At high Q(2) electroweak effects of the heavy bosons Z(o) and W are observed and found to be consistent with Standard Model expectation
MH - Australia
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 98
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000087049900004
L2 - DEEP-INELASTIC-SCATTERING; LIQUID ARGON CALORIMETER; W-BOSON MASS; STRUCTURE-FUNCTION F-2(X,Q(2)); PARTON DISTRIBUTIONS; EP SCATTERING; KINEMATIC RECONSTRUCTION; RADIATIVE-CORRECTIONS; E(+)E(-) COLLISIONS; LEADING ORDER
SO - European Physical Journal C 2000 ;13(4):609-639
34
UI - 16046
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Behrend HJ
AU - Beier C
AU - Belousov A
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bertrand-Coremans G
AU - Biddulph P
AU - Bizot JC
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Buniatian A
AU - Burke S
AU - Burrage A
AU - Buschhorn G
AU - Calvet D
AU - Campbell AJ
AU - Carli T
AU - Chabert E
AU - Charlet M
AU - Clarke D
AU - Clerbaux B
AU - Contreras JG
AU - Cormack C
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - De Roeck A
AU - De Wolf EA
AU - Delcourt B
AU - Demirchyan R
AU - Diaconu C
AU - Dirkmann M
AU - Dixon P
AU - Dlugosz W
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Ebert J
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Elsen E
AU - Enzenberger M
AU - Erdmann M
AU - Fahr AB
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Feltesse J
AU - Ferencei J
AU - Ferrarotto F
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Gaede F
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Gorelov I
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Griffiths RK
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Hampel M
AU - Haustein V
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herynek I
AU - Hewitt K
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoffmann D
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Jonsson L
AU - Johnson DP
AU - Jones M
AU - Jung H
AU - Kastli HK
AU - Kander M
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnik O
AU - Katzy J
AU - Kaufmann O
AU - Kausch M
AU - Keller N
AU - Kenyon IR
AU - Kermiche S
AU - Keuker C
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Kohne JH
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Kramerkamper T
AU - Krasny MW
AU - Krehbiel H
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuster H
AU - Kuhlen M
AU - Kurca T
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Langenegger U
AU - Lebedev A
AU - Lehner F
AU - Lemaitre V
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobo G
AU - Lobodzinska E
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - McMahon TR
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon M
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller D
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Newman PR
AU - Nguyen HK
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Niedzballa C
AU - Niggli H
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Oberlack H
AU - Olsson JE
AU - Ozerov D
AU - Palmen P
AU - Panassik V
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Pawletta H
AU - Perez E
AU - Phillips JP
AU - Pieuchot A
AU - Pitzl D
AU - Poschl R
AU - Pope G
AU - Povh B
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyDESY, Inst Hochenergiephys, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandHumboldt Univ, Inst Phys, Berlin, GermanyBerg Univ Gesamthsch Wuppertal, Rech Zentrum, Wuppertal, GermanyUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Ap, Merida, Yucatan, MexicoRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandInteruniv Inst High Energies ULB VUB, Brussels, BelgiumUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Phys Nucl, Krakow, PolandUniv Calif Davis, Dept Phys, Davis, CA 95616, USAUniv Calif Davis, IIRPA, Davis, CA 95616, USAUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Nucl Res Inst, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Inst Hochenergiephys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Aix Marseille 2, IN2P3, CNRS, CPPM, F-13284 Marseille 07, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, LAL, IN2P3, CNRS, Orsay, FranceEcole Polytech, CNRS, IN2P3, LPNHE, F-91128 Palaiseau, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Nucl Ctr, Prague, Czech RepublicUniv Roma 3, Dipartimento Fis, Rome, ItalyUniv Roma 3, INFN Roma 1, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - Elastic electroproduction of rho mesons at HERA
AB - The elastic electroproduction of rho mesons is studied at HERA with the H1 detector for a photon virtuality in the range 1 < Q(2) < 60 GeV2 and for a hadronic centre of mass energy in the range 30 < W < 140 GeV. The shape of the (pi pi) mass distribution in the rho resonance region is measured as a function of Q(2). The full set of rho spin density matrix elements is determined, and evidence is found for a helicity flip amplitude at the level of 8 +/- 3% of the non-flip amplitudes. Measurements are presented of the dependence of the cross section on Q(2), W and t (the four-momentum transfer squared to the proton). They suggest that, especially at large Q(2), the gamma*p cross section develops a stronger W dependence than that expected from the behaviour of elastic and total hadron-hadron cross sections
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
MH - USA
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 86
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000086888100001
L2 - DIFFRACTIVE PRODUCTION; VECTOR-MESONS; LARGE Q(2); PHOTOPRODUCTION; DISTRIBUTIONS; MUOPRODUCTION; CALORIMETER; SCATTERING; PHYSICS; QCD
SO - European Physical Journal C 2000 ;13(3):371-396
35
UI - 16047
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel T
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Behrend HJ
AU - Beier C
AU - Belousov A
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bertrand-Coremans G
AU - Biddulph P
AU - Bizot JC
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Buniatian A
AU - Burke S
AU - Burrage A
AU - Buschhorn G
AU - Calvet D
AU - Campbell AJ
AU - Carli T
AU - Chabert E
AU - Charlet M
AU - Chyla J
AU - Clarke D
AU - Clerbaux B
AU - Contreras JG
AU - Cormack C
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - De Roeck A
AU - De Wolf EA
AU - Delcourt B
AU - Demirchyan R
AU - Diaconu C
AU - Dirkmann M
AU - Dixon P
AU - Dlugosz W
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Ebert J
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Elsen E
AU - Enzenberger M
AU - Erdmann M
AU - Fahr AB
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Feltesse J
AU - Ferencei J
AU - Ferrarotto F
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Gaede F
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Gorelov I
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Griffiths RK
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Hampel M
AU - Haustein V
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herynek I
AU - Hewitt K
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoffmann D
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Jonsson L
AU - Johnson DP
AU - Jones M
AU - Jung H
AU - Kastli HK
AU - Kander M
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnik O
AU - Katzy J
AU - Kaufmann O
AU - Kausch M
AU - Keller N
AU - Kenyon IR
AU - Kermiche S
AU - Keuker C
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Kohne JH
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Kramerkamper T
AU - Krasny MW
AU - Krehbiel H
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuster H
AU - Kuhlen M
AU - Kurca T
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Langenegger U
AU - Lebedev A
AU - Lehner F
AU - Lemaitre V
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobo G
AU - Lobodzinska E
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - McMahon TR
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon M
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller D
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Newman PR
AU - Nguyen HK
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Niedzballa C
AU - Niggli H
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Oberlack H
AU - Olsson JE
AU - Ozerov D
AU - Palmen P
AU - Panassik V
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Pawletta H
AU - Perez E
AU - Phillips JP
AU - Pieuchot A
AU - Pitzl D
AU - Poschl R
AU - Pope G
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyDESY, Inst Hochenergiephys, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandHumboldt Univ, Inst Phys, Berlin, GermanyBerg Univ Gesamthsch Wuppertal, Rech Zentrum, Wuppertal, GermanyUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Ap, Merida, Yucatan, MexicoRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandInteruniv Inst High Energies ULB VUB, Brussels, BelgiumUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Phys Nucl, Krakow, PolandUniv Calif Davis, IIRPA, Davis, CA 95616, USAUniv Calif Davis, Dept Phys, Davis, CA 95616, USAUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Nucl Res Inst, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Inst Hochenergiephys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Aix Marseille 2, IN2P3, CNRS, CPPM, F-13284 Marseille 07, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, IN2P3, CNRS, LAL, Orsay, FranceEcole Polytech, IN2P3, CNRS, LPNHE, Palaiseau, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Nucl Ctr, Prague, Czech RepublicUniv Roma 3, Dipartimento Fis, Rome, ItalyUniv Roma 3, INFN Roma 1, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - Measurement of dijet cross-sections in low Q(2) ep collisions and the extraction of an effective parton density for the virtual photon
AB - The triple-differential dijet cross-section, d(3)sigma(ep)/dQ(2)d (E) over bar(t)(2) dx(gamma)(jets), is measured with the H1 detector at HERA as a function of the photon virtuality the fraction of the photon's momentum carried by the parton entering the hard scattering, x(gamma)(jets), and the square of the mean transverse energy, (E) over bar(t)(2), of the two highest E-t jets. Jets are found using a longitudinal boost-invariant k(T) clustering algorithm in the gamma*p center of mass frame. The measurements cover the ranges 1.6 < Q(2) < 80 GeV2 in virtuality and 0.1 < y < 0.7 in inelasticity y. The results are well described by leading order QCD models which include the effects of a resolved component to the virtual photon. Models which treat the photon as point-like fail to describe the data. An effective leading order parton density for the virtual photon is extracted as a function of the photon virtuality, the probing scale and the parton momentum fraction. The a:, and probing scale dependences of the parton density show characteristic features of photon structure, and a suppression of this structure with increasing Q(2) is seen
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
MH - USA
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 20
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000086888100002
L2 - LIQUID ARGON CALORIMETER; STRUCTURE-FUNCTION F2; LEADING ORDER; HADRON-COLLISIONS; JET PRODUCTION; PHOTOPRODUCTION; HERA; QCD; SCATTERING; ELECTRON
SO - European Physical Journal C 2000 ;13(3):397-414
36
UI - 16048
AU - Adloff C
AU - Aid S
AU - Anderson M
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Arndt C
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Ban J
AU - Baranov P
AU - Barrelet E
AU - Barschke R
AU - Bartel T
AU - Bassler U
AU - Beck M
AU - Behrend HJ
AU - Beier C
AU - Belousov A
AU - Berger C
AU - Bernardi G
AU - Bertrand-Coremans G
AU - Beyer R
AU - Biddulph P
AU - Bizot JC
AU - Borras K
AU - Boudry V
AU - Bourov S
AU - Braemer A
AU - Braunschweig W
AU - Brisson V
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Brune C
AU - Burger J
AU - Busser FW
AU - Buniatian A
AU - Burke S
AU - Buschhorn G
AU - Calvet D
AU - Campbell AJ
AU - Carli T
AU - Charlet M
AU - Clarke D
AU - Clerbaux B
AU - Cocks S
AU - Contreras JG
AU - Cormack C
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - De Roeck A
AU - De Wolf EA
AU - Delcourt B
AU - Dirkmann M
AU - Dixon P
AU - Dlugosz W
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Ebert J
AU - Ebert TR
AU - Eckerlin G
AU - Efremenko T
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Elsen E
AU - Erdmann M
AU - Fahr AB
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Feltesse J
AU - Ferencei J
AU - Ferrarotto F
AU - Flamm K
AU - Fleischer M
AU - Flieser M
AU - Flugge G
AU - Fomenko A
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Gaede F
AU - Garvey J
AU - Gayler J
AU - Gebauer M
AU - Gerhards R
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Gorelov I
AU - Grab C
AU - Graissler K
AU - Greenshaw T
AU - Griffiths RK
AU - Grindhammer G
AU - Gruber A
AU - Gruber C
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Haller T
AU - Hampel M
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herynek I
AU - Hewitt K
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoppner M
AU - Hoffmann D
AU - Holtom T
AU - Horisberger R
AU - Hudgson VL
AU - Hutte M
AU - Ibbotson M
AU - Issever C
AU - Itterbeck H
AU - Jacquet M
AU - Jaffre M
AU - Janoth J
AU - Jansen DM
AU - Jonsson L
AU - Johnson DP
AU - Jung H
AU - Kalmus PIP
AU - Kander M
AU - Kant D
AU - Karlsson M
AU - Kathage U
AU - Katzy J
AU - Kaufmann HH
AU - Kaufmann O
AU - Kausch M
AU - Kazarian S
AU - Kenyon IR
AU - Kermiche S
AU - Keuker C
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Kohne JH
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Kramerkamper T
AU - Krasny MW
AU - Krehbiel K
AU - Krucker D
AU - Kupper A
AU - Kuster H
AU - Kuhlen M
AU - Kurca T
AU - Laforge B
AU - Lahmann R
AU - Landon MPJ
AU - Lange W
AU - Langenegger U
AU - Lebedev A
AU - Lehner F
AU - Lemaitre V
AU - Levonian S
AU - Lindstroem M
AU - Lipinski J
AU - List B
AU - Lobo G
AU - Lopez GC
AU - Lubimov V
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malinovski E
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martens J
AU - Martin G
AU - Martin R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - McMahon SJ
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Migliori A
AU - Mikocki S
AU - Milstead D
AU - Moeck J
AU - Moreau F
AU - Morris JV
AU - Mroczko E
AU - Muller D
AU - Muller K
AU - Murin H
AU - Nagovizin V
AU - Nahnhauer R
AU - Naroska B
AU - Naumann T
AU - Negri I
AU - Newman RP
AU - Newton D
AU - Nguyen HK
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Niedzballa C
AU - Niggli H
AU - Nowak G
AU - Nunnemann T
AU - Oberlack H
AU - Olsson JE
AU - Ozerov D
AU - Palmen P
AU - Panaro E
AU - Panitch A
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Pawletta H
AU - Peppel E
AU - Perez E
AD - DESY, Inst Hochenergiephys, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandHumboldt Univ, Inst Phys, Berlin, GermanyBerg Univ Gesamthsch Wuppertal, Rech Zentrum, Wuppertal, GermanyUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Ap, Merida, Yucatan, MexicoRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandInteruniv Inst High Energies ULB VUB, Brussels, BelgiumUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Phys Nucl, Krakow, PolandUniv Calif Davis, Dept Phys, Davis, CA 95616, USAUniv Calif Davis, IIRPA, Davis, CA 95616, USAUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Nucl Res Inst, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Inst Hochenergiephys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Aix Marseille 2, IN2P3, CNRS, CPPM, F-13284 Marseille 07, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, IN2P3, CNRS, LAL, Orsay, FranceEcole Polytech, CNRS, IN2P3, LPNHE, F-91128 Palaiseau, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Nucl Ctr, Prague, Czech RepublicUniv Roma 3, Dipartimento Fis, Rome, ItalyUniv Roma 3, INFN Roma 1, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandBerg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyAdloff, C, DESY, Inst Hochenergiephys, Zeuthen, Germany
TI - Di-jet event rates in deep-inelastic scattering at HERA
AB - Di-jet event rates have been measured for deep-inelastic scattering in the kinematic domain 5 less than or similar to Q(2) less than or similar to 100 GeV2 and 10(-4) less than or similar to xBj less than or similar to 10(-2), and for jet transverse moments squared p(t)(*2) greater than or similar to Q(2). The analysis is based on data collected with the H1 detector at HERA in 1994 corresponding to an integrated luminosity of about 2 pb(-1). Jets are defined using a cone algorithm in the photon-proton centre of mass system requiring jet transverse momenta of at least 5 GeV. The di-jet event rates are shown as a function of Q(2) and x(Bj). Leading order models of point-like interacting photons fail to describe the data. Models which add resolved interacting photons or which implement the colour dipole model give a good description of the di-jet event rate. This is also the case for next-to-leading order calculations including contributions from direct and resolved photons
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
MH - USA
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 13
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000086888100003
L2 - MONTE-CARLO GENERATOR; LIQUID ARGON CALORIMETER; PARTON DISTRIBUTIONS; VIRTUAL PHOTON; CROSS-SECTIONS; EP SCATTERING; QCD CASCADES; COLLISIONS; PARTICLES; PHYSICS
SO - European Physical Journal C 2000 ;13(3):415-426
37
UI - 16282
AU - Adloff C
AU - Andreev V
AU - Andrieu B
AU - Arkadov V
AU - Astvatsatourov A
AU - Ayyaz I
AU - Babaev A
AU - Bahr J
AU - Baranov P
AU - Barrelet E
AU - Bartel W
AU - Bassler U
AU - Bate P
AU - Beglarian A
AU - Behnke O
AU - Behrend HJ
AU - Beier C
AU - Belousov A
AU - Berger C
AU - Bernardi G
AU - Berndt T
AU - Bertrand-Coremans G
AU - Biddulph P
AU - Bizot JC
AU - Boudry V
AU - Braunschweig W
AU - Brisson V
AU - Broker HB
AU - Brown DP
AU - Bruckner W
AU - Bruel P
AU - Bruncko D
AU - Burger J
AU - Busser FW
AU - Bunyatyan A
AU - Burke S
AU - Burrage A
AU - Buschhorn G
AU - Calvet D
AU - Campbell AJ
AU - Carli T
AU - Chabert E
AU - Charlet M
AU - Clarke D
AU - Clerbaux B
AU - Contreras JG
AU - Cormack C
AU - Coughlan JA
AU - Cousinou MC
AU - Cox BE
AU - Cozzika G
AU - Cvach J
AU - Dainton JB
AU - Dau WD
AU - Daum K
AU - David M
AU - Davidsson M
AU - De Roeck A
AU - De Wolf EA
AU - Delcourt B
AU - Demirchyan R
AU - Diaconu C
AU - Dirkmann M
AU - Dixon P
AU - Dodonov V
AU - Donovan KT
AU - Dowell JD
AU - Droutskoi A
AU - Ebert J
AU - Eckerlin G
AU - Eckstein D
AU - Efremenko V
AU - Egli S
AU - Eichler R
AU - Eisele F
AU - Eisenhandler E
AU - Elsen E
AU - Enzenberger M
AU - Erdmann M
AU - Fahr AB
AU - Faulkner PJW
AU - Favart L
AU - Fedotov A
AU - Felst R
AU - Feltesse J
AU - Ferencei J
AU - Ferrarotto F
AU - Ferron S
AU - Fleischer M
AU - Flugge G
AU - Fomenko A
AU - Formanek J
AU - Foster JM
AU - Franke G
AU - Gabathuler E
AU - Gabathuler K
AU - Gaede F
AU - Garvey J
AU - Gassner J
AU - Gayler J
AU - Gerhards R
AU - Ghazaryan S
AU - Glazov A
AU - Goerlich L
AU - Gogitidze N
AU - Goldberg M
AU - Gorelov I
AU - Grab C
AU - Grassler H
AU - Greenshaw T
AU - Griffiths RK
AU - Grindhammer G
AU - Hadig T
AU - Haidt D
AU - Hajduk L
AU - Hampel M
AU - Haustein V
AU - Haynes WJ
AU - Heinemann B
AU - Heinzelmann G
AU - Henderson RCW
AU - Hengstmann S
AU - Henschel H
AU - Heremans R
AU - Herrera G
AU - Herynek I
AU - Hewitt K
AU - Hilgers M
AU - Hiller KH
AU - Hilton CD
AU - Hladky J
AU - Hoting P
AU - Hoffmann D
AU - Horisberger R
AU - Hurling S
AU - Ibbotson M
AU - Issever C
AU - Jacquet M
AU - Jaffre M
AU - Janauschek L
AU - Jansen DM
AU - Jonsson L
AU - Johnson DP
AU - Jones M
AU - Jung H
AU - Kastli HK
AU - Kander M
AU - Kant D
AU - Kapichine M
AU - Karlsson M
AU - Karschnick O
AU - Kaufmann O
AU - Kausch M
AU - Keil F
AU - Keller N
AU - Kenyon IR
AU - Kermiche S
AU - Kiesling C
AU - Klein M
AU - Kleinwort C
AU - Knies G
AU - Kohne JH
AU - Kolanoski H
AU - Kolya SD
AU - Korbel V
AU - Kostka P
AU - Kotelnikov SK
AU - Kramerkamper T
AU - Krasny MW
AU - Krehbiel H
AU - Krucker D
AU - Kruger K
AU - Kupper A
AU - Kuster H
AU - Kuhlen M
AU - Kurca T
AU - Lachnit W
AU - Lahmann R
AU - Lamb D
AU - Landon MPJ
AU - Lange W
AU - Langenegger U
AU - Lebedev A
AU - Lehner F
AU - Lemaitre V
AU - Lemrani R
AU - Lendermann V
AU - Levonian S
AU - Lindstroem M
AU - Lobo G
AU - Lobodzinska E
AU - Lubimov V
AU - Luders S
AU - Luke D
AU - Lytkin L
AU - Magnussen N
AU - Mahlke-Kruger H
AU - Malden N
AU - Malinovski E
AU - Malinovski I
AU - Maracek R
AU - Marage P
AU - Marks J
AU - Marshall R
AU - Martyn HU
AU - Martyniak J
AU - Maxfield SJ
AU - McMahon TR
AU - Mehta A
AU - Meier K
AU - Merkel P
AU - Metlica F
AU - Meyer A
AU - Meyer H
AU - Meyer J
AU - Meyer PO
AU - Mikocki S
AU - Milstead D
AU - Mohr R
AU - Mohrdieck S
AU - Mondragon MN
AU - Moreau F
AU - Morozov A
AU - Morris JV
AU - Muller D
AU - Muller K
AU - Murin P
AU - Nagovizin V
AU - Naroska B
AU - Naumann J
AU - Naumann T
AU - Negri I
AU - Newman PR
AU - Nguyen HK
AU - Nicholls TC
AU - Niebergall F
AU - Niebuhr C
AU - Niedzballa C
AU - Niggli H
AU - Nix O
AU - Nowak G
AU - Nunnemann T
AU - Oberlack H
AU - Olsson JE
AU - Ozerov D
AU - Palmen P
AU - Panassik V
AU - Pascaud C
AU - Passaggio S
AU - Patel GD
AU - Pawletta H
AU - Perez E
AU - Phillips JP
AU - Pieuchot A
AU - Pitzl D
AD - Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyRhein Westfal TH Aachen, Inst Phys 1, D-5100 Aachen, GermanyRhein Westfal TH Aachen, Inst Phys 3, D-5100 Aachen, GermanyUniv Birmingham, Sch Phys & Space Res, Birmingham B15 2TT, W Midlands, EnglandUniv Instelling Antwerp, B-2610 Wilrijk, BelgiumULB VUB, Interuniv Inst High Energies, Brussels, BelgiumRutherford Appleton Lab, Didcot OX11 0QX, Oxon, EnglandInst Nucl Phys, Krakow, PolandUniv Dortmund, Inst Phys, D-4600 Dortmund, GermanyJoint Inst Nucl Res, Dubna, RussiaCEA Saclay, DAPNIA, DSM, F-91191 Gif Sur Yvette, FranceDESY, D-2000 Hamburg, GermanyUniv Hamburg, Inst Expt Phys 2, D-2000 Hamburg, GermanyMax Planck Inst Kernphys, D-69117 Heidelberg, GermanyUniv Heidelberg, Inst Phys, D-6900 Heidelberg, GermanyUniv Heidelberg, Inst Hochenergirphys, D-6900 Heidelberg, GermanyUniv Kiel, Inst Expt & Angew Phys, Kiel, GermanySlovak Acad Sci, Inst Expt Phys, Kosice 04353, SlovakiaUniv Lancaster, Sch Phys & Chem, Lancaster, EnglandUniv Liverpool, Dept Phys, Liverpool L69 3BX, Merseyside, EnglandUniv London Queen Mary & Westfield Coll, London E1 4NS, EnglandUniv Lund, Dept Phys, Lund, SwedenUniv Manchester, Dept Phys & Astron, Manchester, Lancs, EnglandUniv Aix Marseille 3, CPPM, IN2P3, CNRS, Marseille, FranceInst Theoret & Expt Phys, Moscow 117259, RussiaPN Lebedev Phys Inst, Moscow 117924, RussiaMax Planck Inst Phys, D-80805 Munich, GermanyUniv Paris Sud, LAL, IN2P3, CNRS, Orsay, FranceEcole Polytech, LPNHE, IN2P3, CNRS, Palaiseau, FranceUniv Paris 06, CNRS, IN2P3, LPNHE, Paris, FranceUniv Paris 07, CNRS, IN2P3, LPNHE, Paris, FranceAcad Sci Czech Republ, Inst Phys, Prague, Czech RepublicCharles Univ, Nucl Ctr, Prague, Czech RepublicUniv Roma 3, INFN Roma 1, Rome, ItalyUniv Roma 3, Dipartimento Fis, Rome, ItalyPaul Scherrer Inst, Villigen, SwitzerlandBerg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, GermanyDESY, Zeuthen, GermanyETH Zurich, Inst Teilchenphys, Zurich, SwitzerlandUniv Zurich, Inst Phys, Zurich, SwitzerlandHumboldt Univ, Inst Phys, Berlin, GermanyBerg Univ Gesamthsch Wuppertal, Rech Zentrum, Wuppertal, GermanyYerevan Phys Inst, Yerevan 375036, ArmeniaUniv Karlsruhe, Inst Expt Kernphys, D-7500 Karlsruhe, GermanyCINVESTAV, Dept Fis Aplicada, Merida, Yucatan, MexicoSafarik Univ, Kosice 04154, SlovakiaAdloff, C, Berg Univ Gesamthsch Wuppertal, Fachbereich Phys, Wuppertal, Germany
TI - Measurements of transverse energy flow in deep-inelastic scattering at HERA
AB - Measurements of transverse energy flow are presented for neutral current deep-inelastic scattering events produced in positron-proton collisions at HERA. the kinematic range covers squared momentum transfers Q(2) from 3.2 to 2 200 GeV2. the Bjorken scaling variable x from 8 . 10(-5) to 0.11 and the hadronic mass W from 66 to 233 GeV. The transverse energy flow is measured in the hadronic centre of mass frame and is studied as a function of Q(2). x, W and pseudorapidity. A comparison is made with QCD-based models. The behaviour of the mean transverse energy in tbe central pseudorapidity region and an interval corresponding to the photon fragmentation region are analysed as a function of Q(2) and W
MH - Armenia
MH - Belgium
MH - Czech Republic
MH - United Kingdom
MH - France
MH - Germany
MH - Italy
MH - Mexico|Yucatan
MH - Poland
MH - Russia
MH - Slovakia
MH - Sweden
MH - Switzerland
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 12
U4 - Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 1434-6044
UR - ISI:000086148700004
L2 - LIQUID ARGON CALORIMETER; INITIAL STATE RADIATION; HADRONIC FINAL-STATE; PERTURBATIVE-QCD; VIRTUAL PHOTON; JET PRODUCTION; SMALL-X; SPECTRA; COLLISIONS; CASCADES
SO - European Physical Journal C 2000 ;12(4):595-607
38
UI - 14639
AU - Afraimovich V
AU - Lin WW
AU - Rulkov NF
AD - Univ Autonoma San Luis Potosi, Inst Invest Comunicac Opt, San Luis Potosi 78000, MexicoNatl Tsing Hua Univ, Dept Math, Hsinchu, TaiwanUniv Calif San Diego, Inst Nonlinear Sci, La Jolla, CA 92093, USAAfraimovich, V, Univ Autonoma San Luis Potosi, Inst Invest Comunicac Opt, San Luis Potosi 78000, Mexico
TI - Fractal dimension for poincare recurrences as an indicator of synchronized chaotic regimes
AB - The studies of the phenomenon of chaos synchronization are usually based upon the analysis of the existence of transversely stable invariant manifold that contains an invariant set of trajectories corresponding to synchronous motions. In this paper we develop a new approach that relies on the notions of topological synchronization and the dimension for Poincare recurrences. We show that the dimension of Poincare recurrences may serve as an indicator for the onset of synchronized chaotic oscillations. This indicator is capable of detecting the regimes of chaos synchronization characterized by the frequency ratio p:q
MH - Mexico|San Luis Potosi
MH - Taiwan
MH - USA
PB - SINGAPORE: WORLD SCIENTIFIC PUBL CO PTE LTD
RP - NOT IN FILE
U3 - TC 2
U4 - Mathematics, Interdisciplinary Applications;Multidisciplinary Sciences
U5 - J;Article
AV - English
IS - 0218-1274
UR - ISI:000165985700004
L2 - SYSTEMS
SO - International Journal of Bifurcation and Chaos 2000 ;10(10):2323-2337
39
UI - 15027
AU - Afraimovich V
AU - Schmeling J
AU - Ugalde E
AU - Urias J
AD - UASLP, IICO, San Luis Potosi 78000, MexicoFree Univ Berlin, Fachbereich Math & Informat, D-14195 Berlin, GermanyAfraimovich, V, UASLP, IICO, Alvaro Obregon 64, San Luis Potosi 78000, Mexico
TI - Spectra of dimensions for Poincare recurrences
AB - The spectra of Poincare recurrences for two classes of dynamical systems are obtained in the framework of the Caratheodory construction. One class contains systems which are topologically conjugate to subshifts with the specification property, the other consists of minimal multipermutative symbolic systems. The spectra are shown to be solutions of a non-homogeneous Bowen equation, and their relationship with multifractal spectra of Lyapunov exponents is exposed
MH - Germany
MH - Mexico|San Luis Potosi
PB - SPRINGFIELD: SOUTHWEST MISSOURI STATE UNIV
RP - NOT IN FILE
U3 - TC 8
U4 - Mathematics, Applied;Mathematics
U5 - J;Article
AV - English
IS - 1078-0947
UR - ISI:000090095300011
L2 - dimension theory;Poincare recurrences;multifractal analysis;EXPONENTS; ENTROPY
SO - Discrete and Continuous Dynamical Systems 2000 ;6(4):901-914
40
UI - 15275
AU - Afraimovich V
AU - Chazottes JR
AU - Saussol B
AD - IICO, UASLP, San Luis Potosi 78210, MexicoInst Super Tecn, Dept Matemat, P-1049001 Lisbon, PortugalAfraimovich, V, IICO, UASLP, A Obregon 64, San Luis Potosi 78210, Mexico
TI - Local dimensions for Poincare recurrences
AB - Pointwise dimensions and spectra for measures associated with Poincare recurrences are calculated for arbitrary weakly specified subshifts with positive entropy and for the corresponding special flows. It is proved that the Poincare recurrence for a "typical" cylinder is asymptotically its length. Examples are provided which show that this is not true for some systems with zero entropy. Precise formulas for dimensions of measures associated with Poincare recurrences are derived, which are comparable to Young's formula for the Hausdorff dimension of measures and Abramov's formula for the entropy of special flows
MH - Mexico|San Luis Potosi
MH - Portugal
PB - PROVIDENCE: AMER MATHEMATICAL SOC
RP - NOT IN FILE
U3 - TC 10
U4 - Mathematics
U5 - J;Article
AV - English
IS - 1079-6762
UR - ISI:000089252900001
SO - Electronic Research Announcements of the American Mathematical Society 2000 ;6():64-74
41
UI - 15580
AU - Afraimovich V
AU - Fernandez B
AD - UASLP, Inst Invest Commun Opt, San Luis Potosi, SLP, MexicoCNRS, Ctr Phys Theor, F-13288 Marseille 09, FranceAfraimovich, V, UASLP, Inst Invest Commun Opt, Av Karakorum 1470,Lomas 4ta Secc, San Luis Potosi, SLP, Mexico
TI - Topological properties of linearly coupled expanding map lattices
AB - We study topological aspects of the dynamics of one-dimensional lattices of coupled expanding maps of an interval, the coupling being a convolution by a sequence in e(1)(Z). Some conditions on the local map are given such that the corresponding coupled map lattice, provided the coupling is sufficiently small, has an invariant set in which the symbolic dynamics is described by the product of local symbolic systems. It follows that both periodic orbits and travelling waves of any real velocity are dense in the uniform topology. Furthermore, we develop a renormalization technique in a family of lattices of coupled piecewise affine maps parametrized by the local slope and the coupling. Self-similarity of the dynamics in this family then follows. AMS classification scheme numbers: 37L60
MH - France
MH - Mexico|San Luis Potosi
PB - BRISTOL: IOP PUBLISHING LTD
RP - NOT IN FILE
U3 - TC 11
U4 - Mathematics, Applied;Physics, Mathematical
U5 - J;Article
AV - English
IS - 0951-7715
UR - ISI:000088344200001
SO - Nonlinearity 2000 ;13(4):973-993
42
UI - 15891
AU - Afraimovich V
AU - Maass A
AU - Urias J
AD - Univ Autonoma San Luis Potosi, Inst Invest Comunicac Opt, San Luis Potosi 78000, SLP, MexicoUniv Chile, Dept Ingn Matemat, Santiago, ChileAfraimovich, V, Univ Autonoma San Luis Potosi, Inst Invest Comunicac Opt, San Luis Potosi 78000, SLP, Mexico
TI - Symbolic dynamics for sticky sets in Hamiltonian systems
AB - Hamiltonian systems, possessing an infinite hierarchy of islands-around-islands structure, have sticky sets, sets of all limiting points of islands of stability. A class of symbolic systems, called multipermutative, is introduced to model the dynamics in the sticky (multifractal) sets. Every multipermutative system is shown to consist of a collection of minimal subsystems that are topologically conjugate to adding machines. These subsystems are uniquely ergodic. Sufficient and necessary conditions of topological conjugacy are given. A subclass of sticky sets is constructed for which Hausdorff dimension is found and multifractal decomposition is described
MH - Chile
MH - Mexico|San Luis Potosi
PB - BRISTOL: IOP PUBLISHING LTD
RP - NOT IN FILE
U3 - TC 6
U4 - Mathematics, Applied;Physics, Mathematical
U5 - J;Article
AV - English
IS - 0951-7715
UR - ISI:000087488900006
L2 - RENORMALIZATION
SO - Nonlinearity 2000 ;13(3):617-637
43
UI - 15474
AU - Afraimovich VS
AU - Young TR
AD - IICO UASLP, San Luis Potosi 78000, MexicoOhio Univ, Dept Math, Athens, OH 45701, USAAfraimovich, VS, IICO UASLP, A Obregon 64, San Luis Potosi 78000, Mexico
TI - Multipliers of homoclinic orbits on surfaces and characteristics of associated invariant sets
AB - Suppose that f is a surface diffeomorphism with a hyperbolic fixed point O and this fixed point has a transversal homoclinic orbit. It is well known that in a vicinity of this type of homoclinic there are hyperbolic invariants sets. We introduce smooth invariants for the homoclinic orbit which we carl the multipliers. As an application, we study the influence of the multipliers on numerical invariants of the hyperbolic invariant sets as the vicinity becomes small
MH - Mexico|San Luis Potosi
MH - USA
PB - SPRINGFIELD: SOUTHWEST MISSOURI STATE UNIV
RP - NOT IN FILE
U3 - TC 1
U4 - Mathematics, Applied;Mathematics
U5 - J;Article
AV - English
IS - 1078-0947
UR - ISI:000088669900014
L2 - hyperbolic set;smooth invariant;transversal homoclinic
SO - Discrete and Continuous Dynamical Systems 2000 ;6(3):691-704
44
UI - 15799
AU - Ageev S
AU - Bogatyi S
AU - Jimenez R
AD - UNAM, Inst Matemat, Cuernavaca 62210, Morelos, MexicoBrest State Univ, Dept Math, Brest, ByelarusMoscow State Univ, Mech & Math Fac, Dept Gen Topol & Geometry, Moscow 119899, RussiaAgeev, S, UNAM, Inst Matemat, Av Univ S-N,Lomas Chamilpa, Cuernavaca 62210, Morelos, Mexico
TI - Free equivariant extensors
AB - We prove for a finite group G and a compact metric G-space Y that the conditions (1) Y is an element of LCn-1 boolean AND Cn-1, and (2) Y is an element of G-AE(X), for every normal n-dimensional space X endowed with a free numerable action of the group G, are equivalent. As a corollary we obtain: (A) For the space X endowed with a free action of the finite group G the conditions (1) the space X is normal, dim X less than or equal to n and K (X; G) less than or equal to n + 1, (2) the space X is normal, dimX less than or equal to n and K(X; G) < infinity; (3) G * ... * G is an element of G-AE(X), are equivalent. (B) For a paracompact space X with a free action of the finite group G the inequality K(X; G) less than or equal to dim X + 1 holds. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Byelarus
MH - Mexico|Morelos
MH - Russia
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 0
U4 - Mathematics, Applied;Mathematics
U5 - J;Article
AV - English
IS - 0166-8641
UR - ISI:000087669100002
L2 - free action;free spaces;free equivariant extensors;FIXED-POINTS; SPACES; MAPS
SO - Topology and Its Applications 2000 ;105(2):157-166
45
UI - 15922
AU - Aguiar JA
AU - Tellez DAL
AU - Yadava YP
AU - Ferreira JM
AU - Montarroyos E
AU - Guzman J
AU - Chavira E
AD - Univ Fed Pernambuco, Dept Fis, Lab Supercond, BR-50670901 Recife, PE, BrazilNatl Autonomous Univ Mexico, Inst Invest Mat, Mexico City 04510, DF, MexicoAguiar, JA, Univ Fed Pernambuco, Dept Fis, Lab Supercond, Av Prof Luis de Barros Freire S-N, BR-50670901 Recife, PE, Brazil
TI - Structural and superconducting properties of the composite LaBaCaCu3O7-delta-Ba2HOHfO5.5
AB - We have successfully fabricated HTS - ceramic insulator composite system LaBaCaCu3O7-delta-Ba2HoHfO5.5 in which particles of the superconductor and insulator materials could coexist with well defined separated phases left intact by stringent high-temperature processing conditions. Addition of Ba2HoHfO5.5 did not have any deteriorating effect on the superconducting properties of the LaBaCaCu3O7-delta superconductor. (C) 2000 Published by Elsevier Science B.V. All rights reserved
MH - Brazil
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 0
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0921-4526
UR - ISI:000087311700338
L2 - Ba2HOHfO5.5;(CaLa)(BaLa)(2)Cu3O6+x;superconducting composite
SO - Physica B 2000 ;284():679-680
46
UI - 15473
AU - Aguilar G
AU - Morlon-Guyot J
AU - Trejo-Aguilar B
AU - Guyot JP
AD - IRD, ORSTOM, Lab Biotechnol Microbienne Trop, Montpellier 1, FranceUNAM, Fac Quim, Dept Alimentos & Biotecnol, Mexico City 04510, DF, MexicoGuyot, JP, IRD, ORSTOM, Lab Biotechnol Microbienne Trop, 911 Ave Agropolis,BP 5045, Montpellier 1, France
TI - Purification and characterization of an extracellular alpha-amylase produced by Lactobacillus manihotivorans LMG 18010(T), an amylolytic lactic acid bacterium
AB - This work presents the purification and characterization of an extracellular alpha-amylase (1,4-alpha-D-glucan glucanohydrolase, EC 3.2.1.1) produced by a new lactic acid bacterium: Lactobacillus manihotivorans able to produce L(+) lactic acid from starch. The molecular weight was found to be 135 kDa. The temperature and pH optimum were 55 degrees C and 5.5, respectively, and pI was 3.8. The alpha-amylase had good stability at pH range from 5 to 6 and the enzyme was sensitive to temperature, losing activity within 1 h of incubation at 55 degrees C. Higher thermal stability was observed when the enzyme was incubated in presence of soluble starch, K-m value and activation energy were 3.44 mg/ml and 32.55 kJ/mol, respectively. Amylose was found to be a better substrate than soluble starch and amylopectin. Al3+, Fe3+, and Hg2+ (10 mM) almost completely inhibited the alpha-amylase. (C) 2000 Elsevier Science Inc. All rights reserved
MH - France
MH - Mexico|Distrito Federal
PB - NEW YORK: ELSEVIER SCIENCE INC
RP - NOT IN FILE
U3 - TC 20
U4 - Biotechnology & Applied Microbiology
U5 - J;Article
AV - English
IS - 0141-0229
UR - ISI:000088713200008
L2 - alpha-amylase;lactic acid bacteria;Lactobacillus manihotivorans;starch;cassava sour starch;AMYLOVORUS; PLANTARUM; STRAIN; SILAGE; FISH; A6
SO - Enzyme and Microbial Technology 2000 ;27(6):406-413
47
UI - 15373
AU - Aguilar JF
AU - Lera M
AU - Sheppard CJR
AD - Univ Sydney, Sch Phys A 28, Dept Phys Opt, Sydney, NSW 2006, AustraliaUniv Cagliari, Dipartimento Ingn Meccan, I-09123 Cagliari, ItalyUniv Sydney, Australian Key Ctr Microscopy & Microanal, Sydney, NSW 2006, AustraliaAguilar, JF, Inst Nacl Astrofis Opt & Elect, Santa Maria Tonantzintla, Puebla 72840, Mexico
TI - Imaging of spheres and surface profiling by confocal microscopy
AB - An investigation of the imaging of spheres can aid in understanding details of the surface profiling method of confocal microscopy. The use of semicircular masks to eliminate artifacts in confocal profiling is investigated experimentally. A theoretical treatment of image formation for a spherical object in reflection confocal microscopy is presented. For large spheres a simple approximate theory is described and is shown to be equivalent to application of the Kirchhoff theory for surface scattering; (C) 2000 Optical Society of America OCIS codes: 180.0180, 180.1790, 170.6900, 120.6660
MH - Australia
MH - Italy
MH - Mexico|Puebla
PB - WASHINGTON: OPTICAL SOC AMER
RP - NOT IN FILE
U3 - TC 9
U4 - Optics
U5 - J;Article
AV - English
IS - 0003-6935
UR - ISI:000089024500020
L2 - ROUGH-SURFACE; DARK-FIELD; SCATTERING; APERTURE; RECONSTRUCTION; SYSTEMS; STOP
SO - Applied Optics 2000 ;39(25):4621-4628
48
UI - 15013
AU - Aguilar LK
AU - guilar-Cordova E
AU - Ando D
AU - rmendariz-Borunda J
AU - Burd PR
AU - Butler EB
AU - Carter B
AU - Chiang YL
AU - Glorioso JC
AU - Henderson DR
AU - Jolly D
AU - McKenny GP
AU - Nemunaitis J
AU - Rives M
AU - Scherer S
AU - Woo SLC
AD - Baylor Coll Med, Ctr Cell & Gene Therapy, Houston, TX 77030, USAAdvantagene Inc, San Diego, CA, USACell Genesys Inc, Foster City, CA, USAUniv Guadalajara, CUCS, Inst Mol Biol Med, Guadalajara 44430, Jalisco, MexicoMaxygen Inc, Redwood City, CA, USABaylor Coll Med, Dept Radiat Oncol, Houston, TX 77030, USATargeted Genet Corp, Seattle, WA, USAAventis Gencell, Preclin Oncol, Hayward, CA, USAUniv Pittsburgh, Sch Med, Pittsburgh, PA, USACalydon Inc, Sunnyvale, CA, USAChiron Corp, Ctr Gene Therapy, San Diego, CA, USARice Univ, Dept Religious Studies, Houston, TX 77251, USAUS Oncol, Dallas, TX, USABaylor Coll Med, Human Genome Sequencing Ctr, Houston, TX 77030, USAAcad Press, Mol Therapy, New York, NY, USACUNY Mt Sinai Sch Med, Inst Gene Therapy & Mol Med, New York, NY 10029, USAAguilar-Cordova, E, Baylor Coll Med, Ctr Cell & Gene Therapy, 1102 Bates St,Suite 1170, Houston, TX 77030 USA
TI - A prescription for gene therapy
MH - Mexico|Jalisco
MH - USA
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 3
U4 - Biotechnology & Applied Microbiology;Genetics & Heredity;Medicine, Research & Experimental
U5 - J;Editorial Material
AV - English
IS - 1525-0016
UR - ISI:000090048100002
SO - Molecular Therapy 2000 ;1(5):385-388
49
UI - 15682
AU - Aguilar S
AU - Tritlla J
AU - Hafid A
AU - Julivert M
AU - Arboleya ML
AU - Saidi A
AD - Natl Autonomous Univ Mexico, Inst Geol, Dept Geoquim, Mexico City 04510, DF, MexicoUniv Autonoma Barcelona, Fac Ciencies, Dept Geol, Unitat Geotecton, Bellaterra, SpainUniv Cadi Ayyad, Fac Sci & Tech, Dept Geol, Marrakech, MoroccoTritlla, J, Natl Autonomous Univ Mexico, Inst Geol, Dept Geoquim, Circuito Invest Cient,Ciudad Univ, Mexico City 04510, DF, Mexico
TI - Geotectonic significance of the textural evolution of fluid inclusions in Precambrian quartz veins from the "Boutonniere de Zenaga" (Anti-Atlas, Morocco)
AB - In the Precambrian Zenaga inlier (boutonniere) in the Anti-Atlas of Morocco, many quartz veins crosscut the Ebournian (Precambrian) basement. The quartz veins predate the deposition of the overlying Precambrian III units, and were probably the feeding channels for the overlying jasperoid formation. The fluid inclusion microthermometry and textural studies show the evolution in a single crystal, from intensely recrystallized inclusions to almost untouched ones recording the uplift of the Ebournian basement. The uplift provoked the over-pressure of the inner fluid inclusions and their "explosion", giving rise to "hook-like" or "decrepitation cluster" textures, while the fluid inclusions located in the outer zones only show necking-down phenomena. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Distrito Federal
MH - Morocco
MH - Spain
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 0
U4 - Geochemistry & Geophysics
U5 - J;Article
AV - English
IS - 0375-6742
UR - ISI:000088104900067
L2 - Precambrian fluids;re-crystallization;fluid inclusion textures;uplifting;Zenaga;Anti-Atlas;Morocco;REEQUILIBRATION
SO - Journal of Geochemical Exploration 2000 ;69():363-368
50
UI - 15917
AU - Aguilera EF
AU - Kolata JJ
AU - Nunes FM
AU - Becchetti FD
AU - DeYoung PA
AU - Goupell M
AU - Guimaraes V
AU - Hughey B
AU - Lee MY
AU - Lizcano D
AU - Martinez-Quiroz E
AU - Nowlin A
AU - O'Donnell TW
AU - Peaslee GF
AU - Peterson D
AU - Santi P
AU - White-Stevens R
AD - Inst Nacl Invest Nucl, Dept Acelerador, Mexico City 11801, DF, MexicoUniv Notre Dame, Dept Phys, Notre Dame, IN 46556, USAInst Super Tecn, Ctr Multidisciplinar Astrofis, P-1096 Lisbon, PortugalUniv Fernando Pessoa, Dept Sci & Technol, P-4200 Oporto, PortugalUniv Michigan, Dept Phys, Ann Arbor, MI 48109, USAHope Coll, Dept Phys, Holland, MI 49422, USAHope Coll, Dept Chem, Holland, MI 49422, USAAguilera, EF, Inst Nacl Invest Nucl, Dept Acelerador, AP 18-1027, Mexico City 11801, DF, Mexico
TI - Transfer and/or breakup modes in the He-6+Bi-209 reaction near the Coulomb barrier
AB - Reaction products from the interaction of He-6 with Bi-209 have been measured at energies near the Coulomb barrier. A He-4 group of remarkable intensity, which dominates the total reaction cross section, has been observed. The angular distribution of the group suggests that it results primarily from a direct nuclear process. it is likely that this transfer and/or breakup channel is the doorway state that accounts for the previously observed large sub-barrier fusion enhancement in this system
MH - Mexico|Distrito Federal
MH - Portugal
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 93
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0031-9007
UR - ISI:000087266300007
L2 - HEAVY-ION FUSION; HALO NUCLEI; ENERGIES; LI-11; HE-6
SO - Physical Review Letters 2000 ;84(22):5058-5061
51
UI - 13855
AU - Aguirre H
AU - Lombarte A
AD - CSIC, Inst Ciencias Mar, E-08039 Barcelona, SpainMazatlan INP, Ctr Reg Invest Pesquera, Sinaloa, MexicoLombarte, A, CSIC, Inst Ciencias Mar, Passeig Joan Borbo S-N, E-08039 Barcelona, Spain
TI - Distribution pattern of taste buds along hyoidal barbels of Mullus barbatus and M-surmuletus
AB - The external taste buds of bony fishes are differentiated and grouped throughout the body epithelium, concentrating in the buccopharyngeal cavity or in certain external organs such as the lips, barbers or fins, The family Mullidae (goatfishes) is characterized by having barbels covered with taste buds (TBs). However, It is not known how the TBs are distributed and how their characteristics vary along the barbels, To obtain answers to these questions, the morphological variability in taste bud density (delta (TB)), pore area (A(p)) and taste bud area (A(TB)) was studied in Mullus barbatus (L,, 1758) (red mullet) and NI. surmuletus (L., 1758) (striped red mullet), for fish ranging in size from 58 to 227 and from 56 to 287 mm in total length (L-T), respectively. Assuming that larger fish are older, in both species the pore area (A(p)) and taste bud area (A(TB)) increased with ontogenic development. Also, in both species clear differences were observed along the barbel, The delta (TB) increased from the basal area to the apical area, whereas both the A(p) and A(TB) had an inverse pattern. Copyright (C) 2001 S. Karger AG, Basel
MH - Mexico|Sinaloa
MH - Spain
PB - BASEL: KARGER
RP - NOT IN FILE
U3 - TC 1
U4 - Behavioral Sciences;Neurosciences
U5 - J;Article
AV - English
IS - 0006-8977
UR - ISI:000168330900004
L2 - external taste buds;morphological variability;density;pore area and taste bud area;fish;hyoidal barbels;MERLUCCIUS; GADIFORMES; TELEOSTEI; MULLIDAE; FISH; HAKE
SO - Brain Behavior and Evolution 2000 ;56(6):323-329
52
UI - 15459
AU - Aguirre NM
AU - de la Cruz GG
AU - Gurevich YG
AU - Logvinov GN
AU - Kasyanchuk MN
AD - Inst Politecn Nacl, Ctr Invest & Estudios Avanzados, Dept Fis, Mexico City 07000, DF, MexicoTernopil Acad Natl Econ, Dept Special Natl Econ, Ternopil, UkraineAguirre, NM, Inst Politecn Nacl, Ctr Invest & Estudios Avanzados, Dept Fis, Apartado Postal 17-740, Mexico City 07000, DF, Mexico
TI - Heat diffusion in two-layer structures: Photoacoustic experiments
AB - The effective thermal conductivity and thermal diffusivity of a two-layer system are investigated from the theoretical point of view for application to photoacoustic experiments. The effective thermal parameters are obtained by comparing the temperature distribution on the left or right surface of the layered structure and some effective one-layer material. These effective thermal parameters are calculated for some special cases as for example, low and high chopper frequency. The influence of the interface thermal contact between the layers plays an important role on the effective thermal parameters. It is shown that the effective thermal conductivity and thermal diffusivity depend strongly upon the used photothermal technique
MH - Mexico|Distrito Federal
MH - Ukraine
PB - BERLIN: WILEY-V C H VERLAG GMBH
RP - NOT IN FILE
U3 - TC 8
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0370-1972
UR - ISI:000088768800140
L2 - 2-LAYER SYSTEM
SO - Physica Status Solidi B-Basic Research 2000 ;220(1):781-787
53
UI - 15277
AU - Agundis C
AU - Pereyra A
AU - Zenteno R
AU - Brassart C
AU - Sierra C
AU - Vazquez L
AU - Zenteno E
AD - Univ Nacl Autonoma Mexico, Fac Med, Dept Bioquim, Lab Inmunol, Mexico City 04510, DF, MexicoUniv Lille 1, Chim Biol Lab, F-59655 Villeneuve Dascq, FranceUMR CNRS 58650, F-59655 Villeneuve Dascq, FranceUniv Autonoma Estado Morelos, Ctr Invest Quim, Lab Lectinas, Cuernavaca 62210, Morelos, MexicoAgundis, C, Univ Nacl Autonoma Mexico, Fac Med, Dept Bioquim, Lab Inmunol, POB 70 159, Mexico City 04510, DF, Mexico
TI - Quantification of lectin in freshwater prawn (Macrobrachium rosenbergii) hemolymph by ELISA
AB - An enzyme-linked immunoabsorbent assay was developed to quantify the lectin present in the hemolymph of the freshwater prawn Macrobrachium rosenbergii. This method involves the use of murine monoclonal IgG1 with kappa light chain (designated as 3G1) antibodies raised against the purified lectin, the assay that we developed recognized as little as 30 ng/ml of lectin, and was used to measure the lectin concentration in animals at different maturation stages. The highest concentration of lectin was identified in the hemolymph from post-larval prawns and the lowest in molt stage adult animals. The hemagglutination activity of the lectin was four-fold higher in adult than in juvenile specimens, although in all cases N-acetylated sugar residues, such as N-acetyl-D-glucosamine, N-acetyl-D-galactosamine, and N-acetyl-D-neuraminic acid were inhibitors of the lectin activity, suggesting that lectin plays a role in the transport of N-acetylated sugar in juvenile prawns. Our results indicate that lectin concentration and hemagglutinating activity could be influenced by developmental conditions of the freshwater prawn. (C) 2000 Elsevier Science Inc. All rights reserved
MH - France
MH - Mexico|Distrito Federal
MH - Mexico|Morelos
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 4
U4 - Biochemistry & Molecular Biology;Zoology
U5 - J;Article
AV - English
IS - 0305-0491
UR - ISI:000089335000004
L2 - Macrobrachium rosenbergii;sialic acid specific lectin;crustacean lectin;developmental regulation;ELISA;monoclonal antibodies;RECOGNITION; IMMUNITY; HEMOCYTES; CRUSTACEA; ANTIBODY; PROTEIN; CELLS
SO - Comparative Biochemistry and Physiology B-Biochemistry & Molecular Biology 2000 ;127(2):165-172
54
UI - 15945
AU - Aimone SL
AU - Mirifico MV
AU - Caram JA
AU - Mitnik DG
AU - Piro OE
AU - Castellano EE
AU - Vasini EJ
AD - Natl Univ La Plata, Dept Quim, Fac Ciencias Exactas, INIFTA, RA-1900 La Plata, ArgentinaCIMAV, Dept Polimeros, Chihuahua, MexicoUNLP, Dept Fis, Fac Ciencias Exactas, La Plata, Buenos Aires, ArgentinaUniv Sao Paulo, Inst Fis Sao Carlos, BR-13560 Sao Carlos, SP, BrazilVasini, EJ, Natl Univ La Plata, Dept Quim, Fac Ciencias Exactas, INIFTA, CC 16,Suc 4, RA-1900 La Plata, Argentina
TI - Unexpected production of 2,4,6-triphenyl-1,3,5-triazine in the electroreduction of 3,4-diphenyl-1,2,5-thiadiazole 1-oxide. Theoretical estimation of reactive sites for 1-oxide and 1,1-dioxide 1,2,5-thiadiazoles
AB - 3,4-Diphenyl-1,2,5-thiadiazole 1-oxide (1a) in acetonitrile solution is electroreduced to 2,4,6-triphenyl-1,3,5-triazine and 3,4-diphenyl-1,2,5-thiadiazole. This behavior is very different from that of similar compounds with other oxidation states of the heterocyclic sulfur atom, such as the 1,1-dioxide derivative (2) and the aromatic 3,4-diphenyl thiadiazole parent ring. The Fukui functions were calculated for 1a and 2 to estimate their reactivity, compare their reactive site, and rationalize the divergent electrochemical properties of 1a. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Argentina
MH - Brazil
MH - Mexico|Chihuahua
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 13
U4 - Chemistry, Organic
U5 - J;Article
AV - English
IS - 0040-4039
UR - ISI:000087199400004
L2 - thiadiazoles;electrochemistry;structure-activity;reduction;ACETONITRILE; DERIVATIVES; HYDROLYSIS; SOLVENTS
SO - Tetrahedron Letters 2000 ;41(19):3531-3535
55
UI - 14537
AU - Aitala EM
AU - Amato S
AU - Anjos JC
AU - Appel JA
AU - Ashery D
AU - Banerjee S
AU - Bediaga I
AU - Blaylock G
AU - Bracker SB
AU - Burchat PR
AU - Burnstein RA
AU - Carter T
AU - Carvalho HS
AU - Copty NK
AU - Cremaldi LM
AU - Darling C
AU - Denisenko K
AU - Devmal S
AU - Fernandez A
AU - Fox GF
AU - Gagnon P
AU - Gobel C
AU - Gounder K
AU - Halling AM
AU - Herrera G
AU - Hurvits G
AU - James C
AU - Kasper PA
AU - Kwan S
AU - Langs DC
AU - Leslie J
AU - Lundberg B
AU - Magnin J
AU - MayTal-Beck S
AU - Meadows B
AU - Neto JRTD
AU - Milburn RH
AU - de Miranda JM
AU - Napier A
AU - Nguyen A
AU - d'Oliveira AB
AU - O'Shaughnessy K
AU - Peng KC
AU - Perera LP
AU - Purohit MV
AU - Quinn B
AU - Radeztsky S
AU - Rafatian A
AU - Reay NW
AU - Reidy JJ
AU - dos Reis AC
AU - Rubin HA
AU - Sanders DA
AU - Santha AKS
AU - Santoro AFS
AU - Schwartz AJ
AU - Sheaff M
AU - Sidwell RA
AU - Simao FRA
AU - Slaughter AJ
AU - Sokoloff MD
AU - Solano J
AU - Stanton NR
AU - Stenson K
AU - Summers DJ
AU - Takach S
AU - Thorne K
AU - Tripathi AK
AU - Watanabe S
AU - Weiss-Babai R
AU - Wiener J
AU - Witchey N
AU - Wolin E
AU - Yi D
AU - Yoshida S
AU - Zaliznyak R
AU - Zhang C
AD - Univ Mississippi, University, MS 38677, USACtr Brasileiro Pesquisas Fis, Rio De Janeiro, BrazilUniv Calif Santa Cruz, Santa Cruz, CA 95064, USAUniv Cincinnati, Cincinnati, OH 45221, USACINVESTAV, Mexico City 14000, DF, MexicoFermilab, Batavia, IL 60510, USAIIT, Chicago, IL 60616, USAKansas State Univ, Manhattan, KS 66506, USAUniv Massachusetts, Amherst, MA 01003, USAPrinceton Univ, Princeton, NJ 08544, USAUniv Autonoma Puebla, Mexico City, DF, MexicoUniv S Carolina, Columbia, SC 29208, USAStanford Univ, Stanford, CA 94305, USATel Aviv Univ, IL-69978 Tel Aviv, IsraelTufts Univ, Medford, MA 02155, USAUniv Wisconsin, Madison, WI 53706, USAYale Univ, New Haven, CT 06511, USAAitala, EM, Univ Mississippi, University, MS 38677, USA
TI - Asymmetries in the production of Lambda(0), Xi(-), and Omega(-) hyperons in 500 GeV/c pi(-)-nucleon interactions
AB - Using data from Fermilab fixed-target experiment E791, we have measured particle-antiparticle production asymmetries for Lambda (0), Xi (-), and Omega (-) hyperons in pi (-) -nucleon interactions at 500 GeV/c. The asymmetries are measured as functions of Feynman-x (x(F)) and p(T)(2) over the ranges -0.12 less than or equal to x(F) less than or equal to 0.12 and 0 less than or equal to p(T)(2) less than or equal to 4 (GeV/c)(2). We find substantial asymmetries, even at x(F) = 0. We also observe leading-particle-type asymmetries which qualitatively agree with theoretical predictions. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Brazil
MH - Israel
MH - Mexico|Distrito Federal
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 8
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0370-2693
UR - ISI:000166228400002
L2 - INTRINSIC CHARM; P INTERACTIONS; GEV-C; D+; POLARIZATION; PARTICLES; MESON; MODEL
SO - Physics Letters B 2000 ;496(1-2):9-18
56
UI - 14584
AU - Aitala EM
AU - Amato S
AU - Anjos JC
AU - Appel JA
AU - Ashery D
AU - Banerjee S
AU - Bediaga I
AU - Blaylock G
AU - Bracker SB
AU - Burchat PR
AU - Burnstein RA
AU - Carter T
AU - Carvalho HS
AU - Copty NK
AU - Cremaldi LM
AU - Darling C
AU - Denisenko K
AU - Devmal S
AU - Fernandez A
AU - Fox GF
AU - Gagnon P
AU - Gobel C
AU - Gounder K
AU - Halling AM
AU - Herrera G
AU - Hurvits G
AU - James C
AU - Kasper PA
AU - Kwan S
AU - Langs DC
AU - Leslie J
AU - Lundberg B
AU - Magnin J
AU - MayTal-Beck S
AU - Meadows B
AU - Neto JRTD
AU - Mihalcea D
AU - Milburn RH
AU - de Miranda JM
AU - Napier A
AU - Nguyen A
AU - d'Oliveira AB
AU - O'Shaughnessy K
AU - Peng KC
AU - Perera LP
AU - Purohit MV
AU - Quinn B
AU - Radeztsky S
AU - Rafatian A
AU - Reay NW
AU - Reidy JJ
AU - dos Reis AC
AU - Rubin HA
AU - Sanders DA
AU - Santha AKS
AU - Santoro AFS
AU - Schwartz AJ
AU - Sheaff M
AU - Sidwell RA
AU - Simao FRA
AU - Slaughter AJ
AU - Sokoloff MD
AU - Solano J
AU - Stanton NR
AU - Stefanski RJ
AU - Stenson K
AU - Summers DJ
AU - Takach S
AU - Thorne K
AU - Tripathi AK
AU - Watanabe S
AU - Weiss-Babai R
AU - Wiener J
AU - Witchey N
AU - Wolin E
AU - Yang SM
AU - Yi D
AU - Yoshida S
AU - Zaliznyak R
AU - Zhang C
AD - Ctr Brasileiro Pesquisas Fis, Rio De Janeiro, BrazilUniv Calif Santa Cruz, Santa Cruz, CA 95064, USAUniv Cincinnati, Cincinnati, OH 45221, USACINVESTAV, Mexico City 07000, DF, MexicoFermi Natl Accelerator Lab, Batavia, IL 60510, USAIIT, Chicago, IL 60616, USAKansas State Univ, Manhattan, KS 66506, USAUniv Massachusetts, Amherst, MA 01003, USAUniv Mississippi, University, MS 38677, USAPrinceton Univ, Princeton, NJ 08544, USAUniv Autonoma Puebla, Mexico City, DF, MexicoUniv S Carolina, Columbia, SC 29208, USAStanford Univ, Stanford, CA 94305, USATel Aviv Univ, IL-69978 Tel Aviv, IsraelTufts Univ, Medford, MA 02155, USAUniv Wisconsin, Madison, WI 53706, USAYale Univ, New Haven, CT 06511, USAMagnin, J, Ctr Brasileiro Pesquisas Fis, Rio De Janeiro, Brazil
TI - Asymmetries in the production of Lambda(+)(c) and Lambda(-)(c) baryons in 500 GeV/c pi(-) nucleon interactions
AB - We present a measurement of asymmetries in the production of Lambda (+)(c) and Lambda (-)(c) baryons in 500 GeV/c pi (-)-nucleon interactions from the E791 experiment at Fermilab. The asymmetries were measured as functions of Feynman x (x(F)) and transverse momentum squared (p(T)(2)) using a sample of 1819 +/- 62 Lambda (c)'s observed in the decay channel Lambda (+)(c) --> pK(-)pi (+). We observe more Lambda (+)(c) than Lambda (-)(c) baryons, with an asymmetry of (12.7 +/- 3.4 +/- 1.3)% independent of x(F) and p(T)(2) in our kinematical range (-0.1 less than or equal to x(F) less than or equal to 0.6 and 0.0 less than or equal to p(T)(2) less than or equal to 8.0 (GeV/c)(2)). This Lambda (c) asymmetry measurement is the first with data in both the positive and negative x(F) regions. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Brazil
MH - Israel
MH - Mexico|Distrito Federal
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 16
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0370-2693
UR - ISI:000166098100005
L2 - D+; MESON
SO - Physics Letters B 2000 ;495(1-2):42-48
57
UI - 16606
AU - Aitala EM
AU - Amato S
AU - Anjos JC
AU - Appel JA
AU - Ashery D
AU - Banerjee S
AU - Bediaga I
AU - Blaylock G
AU - Bracker SB
AU - Burchat PR
AU - Burnstein RA
AU - Carter T
AU - Carvalho HS
AU - Copty NK
AU - Cremaldi LM
AU - Darling C
AU - Denisenko K
AU - Devmal S
AU - Fernandez A
AU - Fox GF
AU - Gagnon P
AU - Gobel C
AU - Gounder K
AU - Halling AM
AU - Herrera G
AU - Hurvits C
AU - James C
AU - Kasper PA
AU - Kwan S
AU - Langs DC
AU - Leslie J
AU - Lundberg B
AU - Magnin J
AU - MayTal-Beck S
AU - Meadows B
AU - Neto JRTD
AU - Mihalcea D
AU - Milburn RH
AU - de Miranda JM
AU - Napier A
AU - Nguyen A
AU - d'Oliveira AB
AU - O'Shaughnessy K
AU - Peng KC
AU - Perera LP
AU - Purohit MV
AU - Quinn B
AU - Radeztsky S
AU - Rafatian A
AU - Reay NW
AU - Reidy JJ
AU - dos Reis AC
AU - Rubin HA
AU - Sanders DA
AU - Santha AKS
AU - Santoro AFS
AU - Schwartz AJ
AU - Sheaff M
AU - Sidwell RA
AU - Slaughter AJ
AU - Sokoloff MD
AU - Solano J
AU - Stanton NR
AU - Stefanski RJ
AU - Stenson K
AU - Summers DJ
AU - Takach S
AU - Thorne K
AU - Tripathi AK
AU - Watanabe S
AU - Weiss-Babai R
AU - Wiener J
AU - Witchey N
AU - Wolin E
AU - Yang SM
AU - Yi D
AU - Yoshida S
AU - Zaliznyak R
AU - Zhang C
AD - Univ Mississippi Oxford, University, MS 38677, USACtr Brasileiro Pesquisas Fis, Rio De Janeiro, BrazilUniv Calif Santa Cruz, Santa Cruz, CA 95064, USAUniv Cincinnati, Cincinnati, OH 45221, USACINVESTAV, Mexico City 07000, DF, MexicoFermi Natl Accelerator Lab, Batavia, IL 60510, USAIIT, Chicago, IL 60616, USAKansas State Univ, Manhattan, KS 66506, USAUniv Massachusetts, Amherst, MA 01003, USAPrinceton Univ, Princeton, NJ 08544, USAUniv Autonoma Puebla, Puebla 72570, MexicoUniv S Carolina, Columbia, SC 29208, USAStanford Univ, Stanford, CA 94305, USATel Aviv Univ, IL-69978 Tel Aviv, IsraelTufts Univ, Medford, MA 02155, USAUniv Wisconsin, Madison, WI 53706, USAYale Univ, New Haven, CT 06511, USAAitala, EM, Univ Mississippi Oxford, University, MS 38677, USA
TI - Multidimensional resonance analysis of Lambda(+)(c) -> pK(-) pi(+)
AB - We present the results of a five-dimensional resonant amplitude analysis of the Lambda(c)(+) --> pK(-)pi(+) system based on 946 +/- 38 reconstructed decays. These data were produced in 500 GeV/c pi(-)-N interactions by Fermilab experiment E791. We report measurements of the amplitudes for Lambda(c)(+) decay into nonresonant pK(-)pi(+) and to p (K) over bar*(0)(890), Delta(++)(1232)K-, and Lambda(1520)pi(+) and we comment on other possible resonant enhancements. This is the first complete amplitude analysis of the Lambda(c)(+) --> pK(-)pi(+) system. We find that (54.8 +/- 5.5 +/- 3.5)% of the decays are nonresonant, (19.5 +/- 2.6 +/- 1.8)% of the decays are via the (K) over bar*(0) resonance, (18.0 +/- 2.9 +/- 2.9)% of the decays are via the Delta(++) resonance, and (7.7 +/- 1.8 +/- 1.1)% of the decays are via the Lambda(1520) resonance. We find evidence for an increasingly negative polarization of the Lambda(c)(+) baryons as a function of p(T)(2), in agreement with a recent model [W.G.D. Dharmaratna, G.R. Goldstein, Phys. Rev. D 53 (1996) 1073; G.R. Goldstein, hep-ph/9907573] and with a related measurement [M. Jezabek, K. Rybicki, R. Rylko, Phys. Lett. B 286 (1992) 175]. (C) 2000 Published by Elsevier Science B.V. All rights reserved
MH - Brazil
MH - Israel
MH - Mexico|Distrito Federal
MH - Mexico|Puebla
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 2
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0370-2693
UR - ISI:000084909800016
L2 - multidimensional;resonance;Lambda(c);polarization;C+
SO - Physics Letters B 2000 ;471(4):449-459
58
UI - 16611
AU - Al-Falou AA
AU - Ball RC
AU - Larralde H
AD - Univ Warwick, Coventry CV4 7AL, W Midlands, EnglandUNAM, Ctr Ciencias Fis, Cuernavaca, Morelos, MexicoAl-Falou, AA, Univ Warwick, Coventry CV4 7AL, W Midlands, England
TI - Dynamical weight functions for a planar crack
AB - The stress intensity factors are evaluated for a moving planar crack for loadings which vary arbitrarily in time and three dimensions of space. We exploit the adjoint elasticity equation obeyed by the corresponding weight functions, and a new and more universal Wiener-Hopf factorization of the Rayleigh function, this beings the central difficulty in such calculations. For the mode a weight function we give further asymptotic results crucial to a subsequent calculation of crack stability with respect to out-of-plane perturbations
MH - United Kingdom
MH - Mexico|Morelos
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 0
U4 - Physics, Fluids & Plasmas;Physics, Mathematical
U5 - J;Article
AV - English
IS - 1063-651X
UR - ISI:000084935200044
L2 - MOVING CRACK
SO - Physical Review e 2000 ;61(1):298-311
59
UI - 15495
AU - Alarcon GS
AU - Amigo MC
AD - Univ Alabama, Div Clin Immunol Rheumatol, Birmingham, AL 35294, USAUniv Peruana Cayetano Heredia, Lima, PeruUniv Nacl Autonoma Mexico, Mexico City 04510, DF, MexicoInst Nacl Caridol Ignacio Chavez, Mexico City, DF, MexicoAlarcon, GS, Univ Alabama, Div Clin Immunol Rheumatol, MEB 615,1813 6th Ave S, Birmingham, AL 35294 USA
TI - The impact of women in the practice of academic and clinical rheumatology in the Americas
MH - USA
MH - Mexico|Distrito Federal
MH - Peru
PB - TORONTO: J RHEUMATOL PUBL CO
RP - NOT IN FILE
U3 - TC 1
U4 - Rheumatology
U5 - J;Editorial Material
AV - English
IS - 0315-162X
UR - ISI:000088543500002
L2 - MEDICAL-EDUCATION; FACULTY; CAREER; PHYSICIANS; CHALLENGES
SO - Journal of Rheumatology 2000 ;27(8):1827-1829
60
UI - 15430
AU - Alarcon J
AU - Becerra J
AU - Silva M
AD - Natl Autonomous Univ Mexico, Inst Quim, Mexico City 04510, DF, MexicoUniv Bio Bio, Fac Ciencias, Chillan, ChileConcepcion Univ, Fac Ciencias Nat, Dept Bot, Lab Quim Prod Nat, Concepcion 2407, Chile
TI - Insecticidal activities of agarofurans from maytenus disticha (celastraceae)
MH - Chile
MH - Mexico|Distrito Federal
PB - WASHINGTON: AMER CHEMICAL SOC
RP - NOT IN FILE
U3 - TC 0
U4 - Chemistry, Multidisciplinary
U5 - J;Meeting Abstract
AV - English
IS - 0065-7727
UR - ISI:000087246100279
SO - Abstracts of Papers of the American Chemical Society 2000 ;219():U73-U74
61
UI - 15250
AU - Alas OT
AU - Sanchis M
AU - Tkacenko MG
AU - Tkachuk VV
AU - Wilson RG
AD - Univ Sao Paulo, Inst Matemat & Estatist, BR-05315970 Sao Paulo, BrazilUniv Jaume 1, Dept Matemat, Castellon, SpainUniv Autonoma Metropolitana Iztapalapa, Dept Matemat, Mexico City 09340, DF, MexicoTkachuk, VV, Univ Sao Paulo, Inst Matemat & Estatist, Caixa Postal 66281, BR-05315970 Sao Paulo, Brazil
TI - Irresolvable and submaximal spaces: Homogeneity versus sigma-discreteness and new ZFC examples
AB - An example of an irresolvable dense subspace of {0, 1)(c) is constructed in ZFC. We prove that there can be no dense maximal subspace in a product of first countable spaces, while under Booth's Lemma there exists a dense submaximal subspace in [0, 1](c). It is established that under the axiom of constructibility any submaximal Hausdorff space is sigma-discrete. Hence it is consistent that there are no submaximal normal connected spaces. If there exists a measurable cardinal, then there are models of ZFC with non-sigma-discrete maximal spaces. We prove that any homogeneous irresolvable space of non-measurable cardinality is of first category. In particular, any homogeneous submaximal space is strongly sigma-discrete if there are no measurable cardinals. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Brazil
MH - Mexico|Distrito Federal
MH - Spain
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 5
U4 - Mathematics, Applied;Mathematics
U5 - J;Article
AV - English
IS - 0166-8641
UR - ISI:000089320000004
L2 - irresolvable space;sep maximal space;submaximal space;homogeneous space
SO - Topology and Its Applications 2000 ;107(3):259-273
62
UI - 15271
AU - Alas OT
AU - Comfort WW
AU - Garcia-Ferreira S
AU - Henriksen M
AU - Wilson RG
AU - Woods RG
AD - Univ Sao Paulo, BR-05315970 Sao Paulo, BrazilWesleyan Univ, Middletown, CT 06459, USANatl Autonomous Univ Mexico, Inst Matemat, Mexico City 04510, DF, MexicoHarvey Mudd Coll, Claremont, CA 91711, USAUniv Autonoma Metropolitana Iztapalapa, Dept Matemat, Unidad Iztapalapa, Mexico City 09340, DF, MexicoUniv Manitoba, Winnipeg, MB R3T 2N2, Canada
TI - When is vertical bar C(XxY)vertical bar=vertical bar C(X)vertical bar vertical bar C(Y)vertical bar?
AB - Sufficient conditions on the Tychonoff spaces X and Y are found that imply that the equation in the title holds. Sufficient conditions on the Tychonoff space X are found that ensure that the equation holds for every Tychonoff space Y. A series of examples (some using rather sophisticated cardinal arithmetic) are given that witness that these results cannot be generalized much
MH - Brazil
MH - Canada
MH - Mexico|Distrito Federal
MH - USA
PB - HOUSTON: UNIV HOUSTON
RP - NOT IN FILE
U3 - TC 0
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0362-1588
UR - ISI:000089217000006
SO - Houston Journal of Mathematics 2000 ;26(1):83-115
63
UI - 16456
AU - Alberdi E
AU - Lehman M
AU - Torroba R
AU - Garavaglia M
AD - Univ Nacl Sur, Dept Fis, Lab Opt, RA-8000 Bahia Blanca, ArgentinaSofilab SACV, Mexico City, DF, MexicoUniv Nacl La Plata, La Plata, ArgentinaCtr Invest Opt, La Plata, ArgentinaLehman, M, Univ Nacl Sur, Dept Fis, Lab Opt, RA-8000 Bahia Blanca, Argentina
TI - Entropic propagation of Gaussian and super-Gaussian-like beams
AB - An entropic formulation to describe the free propagation of Gaussian beams, in a similar way to the thermodynamic theory is developed. We consider two basic applications: (1) an extension to super-Gaussian-like (SGL) beams, and (2) the effect of lenses (convergent and divergent) on the propagation of Gaussian beams. We are interested in such applications because the SGL profiles are obtained through the convolution product using rectangle and Gaussian functions and so, they can be related to the Gaussian beams. The propagation in the Fresnel and Fraunhofer regions are studied, obtaining the laws for the optical entropy of the system. Also, we include some properties and a brief discussion about the condition under which the beam can be considered as an isolated system. For both applications, the evolution of the characteristic width is derived from the entropic postulates. (C) 2000 Published by Elsevier Science B.V. All rights reserved
MH - Argentina
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 2
U4 - Optics
U5 - J;Article
AV - English
IS - 0030-4018
UR - ISI:000085450600001
L2 - BESSEL BEAMS
SO - Optics Communications 2000 ;175(1-3):1-12
64
UI - 15490
AU - Albiter A
AU - Leon CA
AU - Drew RAL
AU - Bedolla E
AD - McGill Univ, Dept Min & Met Engn, Montreal, PQ H3A 2B2, CanadaUMSNH, Inst Invest Met, Morelia 58000, Michoacan, MexicoDrew, RAL, McGill Univ, Dept Min & Met Engn, MH Wong Bldg,3610 Univ St, Montreal, PQ H3A 2B2, Canada
TI - Microstructure and heat-treatment response of Al-2024/TiC composites
AB - Composites of a commercial Al-2024 alloy reinforced with particulate TiC have been produced by the pressureless melt infiltration route. Infiltration was carried out at 1200 degrees C for 2 h and composite materials containing 52 and 55 vol.% TiC were obtained. The phases other than the matrix and the reinforcement were identified as CuAl2, AlTi3, Ti3AlC, and TiAl3. It was found that the composites were age hardenable after solutionizing at 530 degrees C for 150 min and subsequent natural or artificial ageing at 190 degrees C. Mechanical properties of the composites, as-fabricated and heat-treated, showed a strong dependency on the ceramic content. After heat treatment, the 55% TiC composites showed an increase of hardness from 28.5 to 38.5 HRC; meanwhile ultimate tensile strength increased from 379 to 480 MPa. A similar behavior, as a function of heat treatment, was observed for the composites containing 52% TiC, but the estimated values were lower than those obtained for the 55% TiC composites. Scanning electron microscope (SEM) examination revealed transgranular fracture throughout the CuAl2 agglomerated precipitates in the as-fabricated composites. In the heat-treated conditions, brittle and intergranular fractures were observed. (C) 2000 Elsevier Science S.A. All rights reserved
MH - Canada
MH - Mexico|Michoacan
PB - LAUSANNE: ELSEVIER SCIENCE SA
RP - NOT IN FILE
U3 - TC 16
U4 - Nanoscience & Nanotechnology;Materials Science, Multidisciplinary
U5 - J;Article
AV - English
IS - 0921-5093
UR - ISI:000088628300013
L2 - metal matrix composites;Al-2024 alloy;titanium carbide;heat treatment;microstructure;tensile properties;METAL-MATRIX COMPOSITES; TENSILE PROPERTIES; FRACTURE-BEHAVIOR; CREEP-BEHAVIOR; ALUMINUM-ALLOY; TIC COMPOSITES; AL4C3
SO - Materials Science and Engineering A-Structural Materials Properties Microstructure and Processing 2000 ;289(1-2):109-115
65
UI - 16604
AU - Albores A
AU - Cebrian ME
AU - Dekant W
AU - De Matteis F
AU - az-Barriga F
AU - Barril-Antuna J
AU - Fowler J
AU - Gil L
AU - Jaramillo-Juarez F
AU - King LJ
AU - Olarte G
AU - Ostrosky-Wegman P
AU - Patno RI
AU - Torres-Alanis O
AU - Manno M
AD - Cinvestav IPN, Sect Toxicol Ambiental, Dept Farmacol & Toxicol, Mexico City 07360, DF, MexicoUniv Wurzburg, Inst Pharmacol & Toxicol, D-97070 Wurzburg, GermanyUniv Turin, Inst Pharmacol, Turin, ItalyUniv San Luis Potosi, Fac Med, San Luis Potosi, MexicoUniv Alicante, Fac Med, E-03080 San Juan Alicante, SpainEUROTOX, Beecles, Suffolk, EnglandUniv Chile, Fac Med, Santiago 7, ChileUniv Aguascalientes, Ctr Basic Sci, Aguascalientes, MexicoUniv Surrey, Sch Biol Sci, Guildford GU2 5XH, Surrey, EnglandIPN, Natl Sch Biol Sci, Mexico City, DF, MexicoUNAM, Dept Genet Toxicol, Inst Biomed Invest, Mexico City, DF, MexicoUniv Bosque, Fac Med, Santafe Bogota, ColombiaUniv Nuevo Leon, Fac Med, Dept Pharmacol & Toxicol, Monterrey, NL, MexicoUniv Padua, Inst Occupat Med, Padua, ItalyAlbores, A, Cinvestav IPN, Sect Toxicol Ambiental, Dept Farmacol & Toxicol, Ave IPN 2508, Mexico City 07360, DF, Mexico
TI - Structural improvement of higher education in environmental toxicology in Latin America and Europe
AB - Industrial development has resulted in an increased release of chemicals and other agents into the environment, resulting in damage to the environment as well as increasing the risk of adverse effects on human health. Environmental toxicology (ET) is the discipline responsible for assessing the risks to human health and the environment from the effects of new chemicals and those already present in the environment. The development of human resources in toxicology is therefore a priority in both Latin America (LA) and the European Union (EU), although LA professionals are more involved in risk evaluation than in risk assessment compared to their EU colleagues. A solid background in general toxicology will enable those interested in environmental issues to tackle local problems. Moreover, the increasing globalization of markets and, therefore, of the necessary regulations, requires harmonisation of postgraduate programmes to ensure that risk assessment and management related to the environment are dealt with uniformly and by highly qualified scientists. The Inaugural Meeting of the ALFA-OMET Toxicology', a 2-year programme supported by the European Commission, offered the opportunity to discuss a number of these issues. The present status of existing ET courses in the EU and LA. and the corresponding professional profiles in the two regions were examined, and a harmonized academic curriculum for a postgraduate professional profiles in the two regions were examined, and a harmonized academic curriculum for a postgraduate course in environmental toxicology was developed. Finally, a course programme for toxicology and a specialization in environmental toxicology designed by a panel of experts was discussed, and its relevance as a model for other specialisation programmes was analysed. Exercises such as those performed by ALFA-OMET may be useful not only in promoting discussion for the implementation of national and international professional registers in LA, but also in encouraging the same, ongoing process in the EU. (C) 2000 Elsevier Science Ireland Ltd. FLU rights reserved
MH - Chile
MH - Colombia
MH - United Kingdom
MH - Germany
MH - Italy
MH - Mexico|Aguascalientes
MH - Mexico|Distrito Federal
MH - Mexico|Nuevo Leon
MH - Mexico|San Luis Potosi
MH - Spain
PB - CLARE: ELSEVIER SCI IRELAND LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Toxicology
U5 - J;Article
AV - English
IS - 0378-4274
UR - ISI:000084794400003
L2 - academic harmonization;environmental toxicology;higher education programmes;postgraduate education;professional registration
SO - Toxicology Letters 2000 ;111(3):203-211
66
UI - 16054
AU - Alcala JM
AU - Covino E
AU - Sterzik MF
AU - Schmitt JHMM
AU - Krautter J
AU - Neuhauser R
AD - Osservatorio Astron Capodimonte, I-80131 Naples, ItalyEuropean So Observ, Santiago 19, ChileHamburger Sternwarte, D-21029 Hamburg, GermanyLandessternwarte Konigstuhl, D-69117 Heidelberg, GermanyMax Planck Inst Extraterr Phys, D-85740 Garching, GermanyInst Nacl Astrofis Opt & Elect, Puebla, MexicoAlcala, JM, Osservatorio Astron Capodimonte, I-80131 Naples, Italy
TI - A ROSAT pointed observation of the Chamaeleon II dark cloud
AB - A deep 13.5 ksec ROSAT PSPC pointed observation in the Chamaeleon II (Cha II) cloud is reported. 40 X-ray sources are detected of which 14 can be identified with previously known young stellar objects (YSOs), namely IRAS sources, classical T Tauri stars and weak T Tauri stars. From spectroscopic followup observations, four new weak T Tauri candidates have been found. The X-ray sources are mainly located on the north-east of the cloud and their spatial distribution follows the lanes of the 100 mu m dust emission. Their X-ray properties are similar to those of low-mass PMS stars. None of the protostar candidates in Cha II has been detected in the ROSAT pointed observation, in agreement with the ASCA observations results. The X-ray detection rates indicate that the weak T Tauri stars (WTTS) are less numerous than the classical T Tauri stars (CTTS), contrarily to the findings in Chamaeleon I (Cha I) and other star forming regions where the WTTS may outnumber the CTTS. The latter result could be a consequence of the fact that Cha II is in an earlier evolutionary stage as compared to Cha I, as conjectured by previous studies. The Cha II young stellar objects (YSOs) are, on the average, slightly less X-ray luminous than those in Cha I, but the normalised X-ray luminosity distribution functions of the two regions are not significantly different
MH - Chile
MH - Germany
MH - Italy
MH - Mexico|Puebla
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 14
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-6361
UR - ISI:000086869000025
L2 - surveys;stars : formation;stars : low-mass;stars : pre-main sequence;ISM : individual objects : Chamaeleon clouds;X-rays : stars;T-TAURI STARS; MAIN-SEQUENCE STARS; ALL-SKY SURVEY; X-RAY OBSERVATIONS; CHAMELEON-II; STELLAR POPULATION; FORMING REGION; HR DIAGRAM; IDENTIFICATION; ASSOCIATION
SO - Astronomy and Astrophysics 2000 ;355(2):629-638
67
UI - 16640
AU - Alcala JM
AU - Covino E
AU - Torres G
AU - Sterzik MF
AU - Pfeiffer MJ
AU - Neuhauser R
AD - Osservatorio Astron Capodimonte, I-80131 Naples, ItalyHarvard Smithsonian Ctr Astrophys, Cambridge, MA 02138, USAEuropean So Observ, Santiago 19, ChileUniv Munich, Inst Astron & Astrophys, D-81679 Munich, GermanyInst Nacl Astrofis Opt & Elect, Puebla 72000, MexicoMax Planck Inst Extraterr Phys, D-85740 Garching, GermanyAlcala, JM, Osservatorio Astron Capodimonte, I-80131 Naples, Italy
TI - High-resolution spectroscopy of ROSAT low-mass pre-main sequence stars in Orion
AB - High-resolution spectroscopic observations of the lithium-rich stars found on the basis of the ROSAT: All-Sky Survey (RASS) in the general direction of the Orion star forming region are presented. Different properties are derived from the spectra and analyzed: i) the equivalent widths of the lithium 6708 Angstrom absorption line have been measured and a revision of spectral types has been performed: ii) radial velocities (RV) and projected rotational velocities, v sin i, have been derived by application of cross-correlation techniques. A relatively large number of spectroscopic binaries and of suspected spectroscopic binary and multiple systems are found among the stars in the sample. Based on the strength of the lithium line with respect to young open cluster ZAMS stars of the same spectral type, the pre-main sequence nature is confirmed for more than 70% of the stars in the sample. The interrelation of the derived observational properties, such as kinematics, lithium abundance, age and projected rotational velocity of the stars in the sample are analyzed also in connection with the spatial location of the objects. In particular, the comparison between the kinematics of the stars and that of the gas, provided by the CO and CS molecular emission observations, reveals different degrees of clustering of the stars with respect to the cloud material and different kinematical groups can be distinguished. The sample of RASS lithium-rich stars found in the general direction of Orion appears to be a mixture of true Orion stars and, possibly, stars belonging to the Gould Belt
MH - Chile
MH - Germany
MH - Italy
MH - Mexico|Puebla
MH - USA
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 28
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-6361
UR - ISI:000084835500021
L2 - stars : low-mass, brown dwarfs;stars : pre-main sequence;stars : rotation;techniques : radial velocities;techniques : spectroscopic;X-rays : stars;T-TAURI STARS; EMISSION-LINE STARS; SOLAR-TYPE STARS; ALL-SKY SURVEY; X-RAY OBSERVATIONS; RADIAL-VELOCITIES; MOLECULAR CLOUDS; FORMING REGION; OB ASSOCIATION; DARK CLOUD
SO - Astronomy & Astrophysics 2000 ;353(1):186-202
68
UI - 15553
AU - Alcocer L
AU - Reyes AJ
AU - Velasco M
AD - Gen Hosp, Mexico City, DF, MexicoInst Cardiovasc Theory, Montevideo, UruguayCent Univ Caracas, Vargas Med Sch, Dept Pharmacol, Caracas, Venezuela
TI - Positive response of cognitive function to calcium antagonists
MH - Mexico|Distrito Federal
MH - Uruguay
MH - Venezuela
PB - PHILADELPHIA: LIPPINCOTT WILLIAMS & WILKINS
RP - NOT IN FILE
U3 - TC 0
U4 - Peripheral Vascular Disease
U5 - J;Meeting Abstract
AV - English
IS - 0263-6352
UR - ISI:000087593800548
SO - Journal of Hypertension 2000 ;18():S160-S160
69
UI - 14823
AU - Aleshkevich V
AU - Kartashov Y
AU - Vysloukh V
AD - Moscow MV Lomonosov State Univ, Dept Phys, Chair Gen Phys, Moscow 119899, RussiaUAEM, CIICAp, Cuernavaca 62210, Morelos, MexicoKartashov, Y, Moscow MV Lomonosov State Univ, Dept Phys, Chair Gen Phys, Vorobiovy Gory, Moscow 119899, Russia
TI - Cnoidal waves compression by means of multisoliton effect
AB - We consider the self-compression of the cnoidal waves of both cn- and dn-types in the materials with focusing Kerr nonlinearity. The dependencies of the compression degree and optimal media length on the parameter describing localisation of the wave energy are presented and the main features of the wave propagation are analysed on the basis of finite number harmonic approximation. (C) 2000 Elsevier Science B.V, All rights reserved
MH - Mexico|Morelos
MH - Russia
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 10
U4 - Optics
U5 - J;Article
AV - English
IS - 0030-4018
UR - ISI:000165417300010
L2 - self-compression;cnoidal waves;optical solitons;OPTICAL FIBERS; MODULATION; SOLITONS
SO - Optics Communications 2000 ;185(4-6):305-314
70
UI - 16549
AU - Aleshkevich V
AU - Vysloukh V
AU - Kartashov Y
AD - Moscow MV Lomonosov State Univ, Dept Phys, Chair Gen Phys, Moscow 119899, RussiaUAEM, CIICAp, Cuernavaca 62210, Morelos, MexicoKartashov, Y, Moscow MV Lomonosov State Univ, Dept Phys, Chair Gen Phys, Vorobiovy Gory, Moscow 119899, Russia
TI - Self-bending of cnoidal waves in photorefractive medium with drift and diffusion nonlinearity
AB - We consider the influence of the nonlocal component of the photorefractive crystal response on the cnoidal waves propagation dynamic and analyze the dependence of the self-bending parameter on the degree of the spatial localization of the wave energy. We have shown that for the case of the cn-wave the role of self-bending effects increases (and for the case of the dn-wave decreases) with growth of spatial localization. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Morelos
MH - Russia
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 1
U4 - Optics
U5 - J;Article
AV - English
IS - 0030-4018
UR - ISI:000085132600035
L2 - spatial solitons;photorefractive medium;nonlocal nonlinear response;cnoidal waves;SCHRODINGER-EQUATION; OPTICAL FIBERS; CRYSTALS; SOLITONS
SO - Optics Communications 2000 ;174(1-4):277-284
71
UI - 15870
AU - Alexandrova L
AU - D'yachenko OG
AU - Kazankov GM
AU - Polyakov VA
AU - Samuleev PV
AU - Sansores E
AU - Ryabov AD
AD - Natl Autonomous Univ Mexico, Inst Invest Mat, Mexico City 04510, DF, MexicoMoscow MV Lomonosov State Univ, Dept Chem, Moscow 119899, RussiaDI Mendeleev Moscow Univ Chem Technol, Moscow 125820, RussiaRyabov, AD, Carnegie Mellon Univ, Dept Chem, 4400 5th Ave, Pittsburgh, PA 15213 USA
TI - Mechanism of biologically relevant deoxygenation of dimethyl sulfoxide coupled with Pt(II) to Pt(IV) oxidation of orthoplatinated oximes. Synthetic, kinetic, electrochemical, X-ray structural, and density functional study
AB - Orthometalated aryl oxime complexes cis-(C,S)-[Pt-II(C6H3-2-CMe=NOH-5-R)Cl(Me2S=O)] (1, R = H (a), MeO, Me, F, and Cl) undergo deoxygenation of dimethyl sulfoxide (DMSO) in methanol in the presence of HCl to afford the Pt(IV) dimethyl sulfide complexes fac-[Pt-IV(C6H3-2-CMe=NOH-5-R)Cl-3(Me2S)] (2), the composition of which was confirmed by an X-ray structural study of 2a. The mechanism of the deoxygenation coupled with the oxidation of Pt(II) to Pt(IV) was investigated using cyclic voltammety, UV-vis, and H-1 NMR spectrometry techniques at 40-60 degrees C in the presence of HCl, LiCl, and NaClO4. The conversion of 1 into 2 does not occur intramolecularly and involves two time-resolved phases which were studied independently. The first is the substitution of chloride for DMSO to afford the anionic reactive complexes cis-[Pt(C6H3-2-CMe=NOH-5-R)Cl-2](-) (1(Cl)), which are involved in the acid-promoted interaction with free DMSO in the second phase. The formation of 1(Cl) follows the usual two-term rate law k(obs1) + k(s) + k(Cl)[LiCl], the kcl-driven pathway being negligible for the electron-rich complex with R = MeO. Thus-generated complexes 1(Cl) in contrast to their precursors 1, are more susceptible to oxidation, and the irreversible peak for 1(Cl) E(p1), is observed ca. 300 mV more cathodically compared to that of i. The second phase is acid-catalyzed and at low LiCl concentrations follows the rate expression k(obs2)[H+](-1) = k(10)' + k(10)[LiCl]. The complexes with the electron-withdrawing substituents R react faster, and there is a linear correlation between log k(10) and E(p1). The first-order in the acid is discussed in terms of two kinetically indistinguishable mechanisms involving the rate-limiting either electron transfer from Icl to protonated DMSO (mechanism 1) or insertion of the S=O bond of free DMSO into the platinum-hydride bond of the reactive hydride complex of Pt(IV), cis-[Pt(C6H3-2-CMe=NOH)(H)Cl-2], to afford a {Pt-SMe2-OH} fragment. Its protonation by HCl and dissociation of water fives the final product 2 (mechanism 2). H-1 NMR evidence is presented for the formation of the hydride species on protonation of a Pt(II) complex, whereas a density functional study of the two mechanisms indicates that mechanism 2 is less energy demanding. The system studied is viewed as a functioning mimetic of the Mo-dependent enzyme DMSO reductase because of several common features observed in catalysis
MH - Mexico|Distrito Federal
MH - USA
MH - Russia
PB - WASHINGTON: AMER CHEMICAL SOC
RP - NOT IN FILE
U3 - TC 19
U4 - Chemistry, Multidisciplinary
U5 - J;Article
AV - English
IS - 0002-7863
UR - ISI:000087559700020
L2 - EFFECTIVE CORE POTENTIALS; PLATINUM(II) COMPLEXES; MOLECULAR CALCULATIONS; CRYSTAL-STRUCTURES; METAL-COMPLEXES; METHYL(HYDRIDO)PLATINUM(IV) COMPLEXES; DIMETHYLSULFOXIDE REDUCTASE; REACTIVITY; LIGANDS; ION
SO - Journal of the American Chemical Society 2000 ;122(21):5189-5200
72
UI - 15318
AU - Alfaro EJ
AU - Moreno E
AU - Franco J
AD - CSIC, Inst Astrofis Andalucia, Granada, SpainUniv Nacl Autonoma Mexico, Astron Inst, Mexico City 04510, DF, MexicoAlfaro, EJ, CSIC, Inst Astrofis Andalucia, Apartado 3004, Granada, Spain
TI - Kinematics of Gould's belt: Model and observations
AB - Using the available data for nearby stars we derive the velocity ellipsoid of dwarf O-B5.5 stars belonging to the Gould Belt (GB). The resulting vertex deviation for the whole sample is negative (l(v) approximate to -70 degrees) and this value is modified to l(v) approximate to 20 degrees when the members of the Pleiades moving group are removed from the sample. This implies the existence of, at least, two different kinematic groups defining the GB system. We also model the evolution of a supershell in the solar neighborhood, and obtain a fit to the shape and kinematics of the gas in GB. Assuming that the expanding shell is also forming stars, we obtain the corresponding velocity fields for the shell and its newly formed stars. The average vertex deviation value resulting from these models for the new stars is l(v) approximate to 20 degrees, and is consistent with the observed value when the Pleiades moving group members are excluded from the GB
MH - Mexico|Distrito Federal
MH - Spain
PB - DORDRECHT: KLUWER ACADEMIC PUBL
RP - NOT IN FILE
U3 - TC 0
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-640X
UR - ISI:000089142200008
L2 - HIPPARCOS DATA; MOVING GROUPS; STARS; IDENTIFICATION; SAMPLE; GAS
SO - Astrophysics and Space Science 2000 ;272(1-3):53-59
73
UI - 16391
AU - Alfaro J
AU - Morales-Tecotl HA
AU - Urrutia LF
AD - Pontificia Univ Catolica Chile, Fac Fis, Santiago 22, ChileUniv Autonoma Metropolitana Iztapalapa, Dept Fis, Mexico City 09340, DF, MexicoNatl Autonomous Univ Mexico, Inst Ciencias Nucl, Dept Fis Atlas Energias, Mexico City 04510, DF, MexicoAlfaro, J, Pontificia Univ Catolica Chile, Fac Fis, Casilla 306, Santiago 22, Chile
TI - Quantum gravity corrections to neutrino propagation
AB - Massive spin-1/2 fields are studied in the framework of loop quantum gravity by considering a state approximating, at a length scale L much greater than Planck length ep, a spin-1/2 field in flat spacetime. The discrete structure of spacetime at ep yields corrections to the field propagation at scale L. Neutrino bursts ((p) over bar approximate to 10(5) GeV) accompanying gamma ray bursts that have traveled cosmological distances L are considered. The dominant correction is helicity independent and leads to a time delay of order ((p) over bar lp)L/c approximate to 10(4) s. To next order in (p) over bar lp, the correction has the form of the Gambini and Pullin effect for photons. A dependence L-os(-1) proportional to (p) over bar(2)lp is found for a two-flavor neutrino oscillation length
MH - Chile
MH - Mexico|Distrito Federal
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 144
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0031-9007
UR - ISI:000085791900009
L2 - GAMMA-RAY BURSTS; SPIN DYNAMICS QSD; ENERGY NEUTRINOS; FIELD THEORIES; WEAVE STATES; CONSTRAINT; FERMIONS
SO - Physical Review Letters 2000 ;84(11):2318-2321
74
UI - 15337
AU - Algin A
AU - Arik M
AU - Atakishiyev NM
AD - Osmangazi Univ, Dept Phys, Meselik, Eskisehir, TurkeyBogazici Univ, Dept Phys, Istanbul, TurkeyUniv Nacl Autonoma Mexico, Inst Matemat, Cuernavaca 62191, Morelos, MexicoFeza Gursey Inst, TR-81220 Istanbul, TurkeyAlgin, A, Osmangazi Univ, Dept Phys, Meselik, Eskisehir, Turkey
TI - SU(d)-invariant multidimensional q-oscillators with bosonic degeneracy
AB - Multidimensional two-parameter (q(1),q(2))-oscillators are of two kinds: one is invariant under the (ordinary) Lie group SU(d), whereas the other is invariant under the quantum group SUq(d) where q = q(1)/q(2). It is shown that the q(1) = q(2) limit of both of these two-parameter oscillators coincide and give the q-deformed Newton oscillator which can be derived from the standard quantum harmonic oscillator Newton equation. The bosonic degeneracies of the excited levels of these oscillators are different for q(1) not equal q(2), but coincide in the q(1) = q(2) limit
MH - Mexico|Morelos
MH - Turkey
PB - SINGAPORE: WORLD SCIENTIFIC PUBL CO PTE LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Physics, Nuclear;Physics, Particles & Fields;Physics, Mathematical
U5 - J;Article
AV - English
IS - 0217-7323
UR - ISI:000089044200003
L2 - HARMONIC-OSCILLATOR
SO - Modern Physics Letters A 2000 ;15(19):1237-1242
75
UI - 15100
AU - Ali ST
AU - Atakishiyev NM
AU - Chumakov SM
AU - Wolf KB
AD - Concordia Univ, Dept Math & Stat, Montreal, PQ H4B 1R6, CanadaUNAM, Inst Matemat, Cuernavaca, Morelos, MexicoUniv Guadalajara, Dept Ciencias Basicas, Mexico City, DF, MexicoUniv Nacl Autonoma Mexico, Ctr Ciencias Fis, Cuernavaca 62251, Morelos, MexicoAli, ST, Concordia Univ, Dept Math & Stat, Montreal, PQ H4B 1R6, Canada
TI - The Wigner function for general Lie groups and the wavelet transform
AB - We build Wigner maps, functions and operators on general phase spaces arising from a class of Lie groups, including non-unimodular groups (such as the affine group). The phase spaces are coadjoint orbits in the dual of the Lie algebra of these groups and they come equipped with natural symplectic structures and Liouville-type invariant measures. When the group admits square-integrable representations, we present a very general construction of a Wigner function which enjoys all the desirable properties, including full covariance and reconstruction formulae. We study in detail the case of the affine group on the line. In particular, we put into focus the close connection between the well-known wavelet transform and the Wigner function on such groups
MH - Canada
MH - Mexico|Distrito Federal
MH - Mexico|Morelos
PB - BASEL: BIRKHAUSER VERLAG AG
RP - NOT IN FILE
U3 - TC 25
U4 - Physics, Multidisciplinary;Physics, Particles & Fields;Physics, Mathematical
U5 - J;Article
AV - English
IS - 1424-0637
UR - ISI:000089774700004
L2 - COHERENT STATES; SYSTEMS; OPTICS
SO - Annales Henri Poincare 2000 ;1(4):685-714
76
UI - 15583
AU - Alieva T
AU - Wolf KB
AD - Ctr Int Ciencias, Cuernavaca 62210, Morelos, MexicoWolf, KB, Eindhoven Univ Technol, Fac Elektrotech, POB 513, NL-5600 MB Eindhoven, Netherlands
TI - Finite mode analysis through harmonic waveguides
AB - The mode analysis of signals in a multimodal shallow harmonic waveguide whose eigenfrequencies are equally spaced and finite can be performed by an optoelectronic device, of which the optical part uses the guide to sample the wave field at a number of sensors along its axis and the electronic part computes their fast Fourier transform. We illustrate this process with the Kravchuk transform. (C) 2000 Optical Society of America [S0740-3232(00)00408-7]
MH - Mexico|Morelos
MH - Netherlands
PB - WASHINGTON: OPTICAL SOC AMER
RP - NOT IN FILE
U3 - TC 1
U4 - Optics
U5 - J;Article
AV - English
IS - 0740-3232
UR - ISI:000088342200015
L2 - FOURIER-TRANSFORM
SO - Journal of the Optical Society of America A-Optics Image Science and Vision 2000 ;17(8):1482-1484
77
UI - 15911
AU - Allen LH
AU - Rosado JL
AU - Casterline JE
AU - Lopez P
AU - Munoz E
AU - Garcia OP
AU - Martinez H
AD - Univ Calif Davis, Dept Nutr, Program Int Nutr, Davis, CA 95616, USAInst Nacl Nutr, Detp Fisiol Nutr, Tlalpan, MexicoNatl Publ Hlth Inst, Mexican Social Secur Inst, Interinst Hlth Serv Res Grp, Cuernavaca, Morelos, MexicoAllen, LH, Univ Calif Davis, Dept Nutr, Program Int Nutr, 1 Shields Ave, Davis, CA 95616 USA
TI - Lack of hemoglobin response to iron supplementation in anemic Mexican preschoolers with multiple micronutrient deficiencies
AB - Background: In developing countries, incomplete resolution of anemia with iron supplementation is often attributed to poor compliance or inadequate duration of supplementation, but it could result from deficiencies of other micronutrients. Objective: Our objective was to assess children's hematologic response to supervised, long-term iron supplementation and the relation of this response to other micronutrient deficiencies, anthropometry, morbidity, and usual dietary intake. Design: Rural Mexican children aged 18-36 mo (n = 219) were supplemented for 12 mo with either 20 mg Fe, 20 mg Zn, both iron and zinc, or placebo. Children were categorized as iron-unsupplemented (IUS; n = 109) or iron supplemented (IS; n = 108). Hemoglobin, hematocrit, mean corpuscular volume, mean cell hemoglobin, plasma concentrations of micronutrients that can affect hematopoiesis, anthropometry, and diet were assessed at 0, 6, and 12 mo; morbidity was assessed biweekly. Results: At baseline, 70% of children had low hemoglobin (less than or equal to 115 g/L), 60% had low hematocrit, 48% were ferritin deficient, 10% had deficient and 33% had low plasma vitamin B-12 concentrations, 29% had deficient vitamin A concentrations, and 70% had deficient vitamin E concentrations. Iron supplementation increased ferritin from 11 +/- 14 mu g/L at baseline to 31 +/- 18 mu g/L after 6 mo (P < 0.001) and 41 +/- 17 mu g/L after 12 mo. How ever, anemia persisted in 30% and 31% of supplemented children at 6 and 12 mo, respectively, and was not significantly different between the IUS and IS groups at 12 mo. Initial plasma vitamin B-12, height-for-age, and dietary quality predicted the hematopoietic response to iron. Conclusion: Lack of hemoglobin response to iron was associated with indicators of chronic undernutrition and multiple micronutrient deficiencies
MH - USA
MH - Mexico|Morelos
MH - Mexico|Distrito Federal
PB - BETHESDA: AMER SOC CLINICAL NUTRITION
RP - NOT IN FILE
U3 - TC 34
U4 - Nutrition & Dietetics
U5 - J;Article
AV - English
IS - 0002-9165
UR - ISI:000087426300017
L2 - iron supplementation;anemia;iron deficiency;vitamin B-12;retinol;tocopherol;anthropometry;dietary quality;children;micronutrient deficiencies;hemoglobin response;Mexico;VITAMIN-A; PREDICTED PREVALENCE; VILLAGE POPULATIONS; CHILDREN; WOMEN; RIBOFLAVIN; INFANTS; MEN; INADEQUACY; TODDLERS
SO - American Journal of Clinical Nutrition 2000 ;71(6):1485-1494
78
UI - 15237
AU - Alonso C
AU - Andrade C
AU - Castellote M
AU - Castro P
AD - CSIC, Inst Construct Sci Eduardo Torroja, Madrid 28033, SpainIPN, Ctr Invest & Estudios Avanzados, Unidad Merida, Merida 97310, Yucatan, MexicoAlonso, C, CSIC, Inst Construct Sci Eduardo Torroja, C Serrano Galvache S-N, Madrid 28033, Spain
TI - Chloride threshold values to depassivate reinforcing bars embedded in a standardized OPC mortar
AB - The chloride threshold to develop active corrosion of the reinforcing steel does not seem to be a unique value and it depends on several factors, such as concrete mix proportions, cement type, C(3)A content of cement, blended materials, water/cement ratio, temperature, relative humidity, steel surface conditions and source of chloride penetration among others. Numerous studies have been already devoted to the study of the chloride threshold value for depassivation of the steel embedded in concrete. One of the reasons found for the scatter is the large number of variables that influence the chloride amount for depassivation. The other reason is the lack of accordance for the definition of the chloride threshold itself, either on the determining parameters (visual observation, corrosion potential or corrosion current) or on the expression of the threshold (as Cl-/OH- ratio or by weight of cement or concrete). The present paper presents chloride thresholds that were studied in mortar based on corrosion current measurements and expressed as total, free and Cl-/OH- ratio. For this study, mainly smoothed bars were used, but also some ribbed bars were tested. Chloride thresholds in the range of 1.24-3.08% and 0.39-1.16%, by weight of cement, for total and free chlorides, respectively, and in the range of 1.17-3.98 for Cl-/OH- ratio were found for chlorides admired in the mixing water Active corrosion is considered when, in a small exposed area, the corrosion rate of the rebar is higher than 0.1 mu A/cm(2). The threshold in the case of Cl-/OH- results a bit higher than that found in a previous work for synthetic pore solution, although the two types of data can be fitted together finding a good correlation. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Mexico|Yucatan
MH - Spain
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 48
U4 - Construction & Building Technology;Materials Science, Multidisciplinary
U5 - J;Article
AV - English
IS - 0008-8846
UR - ISI:000089442800006
L2 - chloride;threshold;corrosion;reinforcement;corrosion rate;PORE SOLUTION CHEMISTRY; CONTAMINATED CONCRETE; CORROSION; STEEL; CEMENT
SO - Cement and Concrete Research 2000 ;30(7):1047-1055
79
UI - 16295
AU - Alonso G
AU - Petranovskii V
AU - del Valle M
AU - Cruz-Reyes J
AU - Licea-Claverie A
AU - Fuentes S
AD - Inst Mexicano Petr, Mexico City 07730, DF, MexicoCtr Invest Mat Avanzados, Chihuahua, Chih, MexicoUniv Autonoma Baja California, Fac Ciencias Quim, Tijuana, BC, CanadaInst Tecnol, Grad Ctr, Tijuana, BC, CanadaFuentes, S, Inst Mexicano Petr, Eje Cent L Cardenas 152,Apdo Postal 14-805, Mexico City 07730, DF, Mexico
TI - Preparation of WS2 catalysts by in situ decomposition of tetraalkylammonium thiotungstates
AB - Tungsten tetraalkylammonium thiosalts are used as precursors for the in situ formation of WS2 catalysts in dibenzothiophene (DBT) hydrodesulfurization. The thermal decomposition of alkyl-ammonium thiosalts proceeds directly to WS2 without WS3 formation, as in the case of ammonium thiotungstate (ATT), allowing good control of the catalyst's stoichiometry, The alkyl-ammonium thiosalts give WS2 particles with different characteristic morphologies. The hydrodesulfurization (HDS) activities of WS2 catalysts derived from alkylthiosalts are higher than those of catalysts derived from the ammonium thiosalt, The reaction rate increases with the size of the cation in the precursor. No correlation of catalytic activities with surface areas is found. The S/W and C/W surface ratios determined by Auger electron spectroscopy decrease with increasing cation size. Surface composition is WS2.25C1.7, WS1.7 C-0.9 and WS1.3 C-0.7 for the in situ catalysts derived from ammonium, methylammonium, and butylammonium precursors, respectively. The improved catalytic properties of WS2 catalysts derived from alkylammonium thiosalts in the HDS of DBT are attributed to the formation of carbon-containing tungsten sulfide phases on the catalyst's surface. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Canada
MH - Mexico|Chihuahua
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 27
U4 - Chemistry, Physical;Environmental Sciences
U5 - J;Article
AV - English
IS - 0926-860X
UR - ISI:000086192900011
L2 - WS2;tetraalkylammonium thiosalts;in situ activation;hydrodesulfurization;TUNGSTEN SULFIDE CATALYSTS; EX AMMONIUM TETRATHIOMOLYBDATE; OXYGEN; HYDRODESULFURIZATION; THIOMOLYBDATES; ALKANES; CARBIDE; CO
SO - Applied Catalysis A-General 2000 ;197(1):87-97
80
UI - 15718
AU - Alonso MA
AD - Macquarie Univ, Dept Phys, Sydney, NSW 2109, AustraliaAlonso, MA, Univ Nacl Autonoma Mexico, Ctr Ciencias Fis, AC, Ctr Int Ciencias, APO 48-3, Cuernavaca 62251, Morelos, Mexico
TI - Measurement of Helmholtz wave fields
AB - A simple formalism is found for the measurement of wave fields that satisfy the Helmholtz equation in free space. This formalism turns out to be analogous to the well-known theory of measurements for quantum-mechanical wave functions: A measurement corresponds to the squared magnitude of the inner product (in a suitable Hilbert space) of the wave field and a field that is associated with the detector. The measurement can also be expressed as an overlap in phase space of a special form of the Wigner function that is tailored for Helmholtz wave fields. (C) 2000 Optical Society of America [S0740-3232(00)00906-6] OCIS codes: 040.0040, 030.5630, 030.1670, 260.0260, 350.7420
MH - Australia
MH - Mexico|Morelos
PB - WASHINGTON: OPTICAL SOC AMER
RP - NOT IN FILE
U3 - TC 6
U4 - Optics
U5 - J;Article
AV - English
IS - 0740-3232
UR - ISI:000087895600013
L2 - WIGNER DISTRIBUTION FUNCTION
SO - Journal of the Optical Society of America A-Optics Image Science and Vision 2000 ;17(7):1256-1264
81
UI - 15861
AU - AlSunaidi A
AU - Lach-hab M
AU - Blaisten-Barojas E
AU - Gonzalez AE
AD - George Mason Univ, Sch COmputat Sci, Fairfax, VA 22030, USAUniv Nacl Autonoma Mexico, Ctr Ciencias Fis, Cuernavaca 62251, Morelos, MexicoAlSunaidi, A, George Mason Univ, Sch COmputat Sci, Fairfax, VA 22030 USA
TI - Colloidal aggregation with mobile impurities
AB - The structure and aggregation kinetics of diffusion-limited cluster-cluster three-dimensional monomeric aggregates and gels is investigated as a function of the molar fraction of two types of impurities. In one case the impurities are allowed to aggregate among themselves whereas in the other the impurities are mobile monomers that remain as such during the whole aggregation process. Computer simulations are performed on a simple cubic lattice for which the functionality of the aggregating particles is effectively 6. The first type of impurity shows a decrease in the fractal dimension when compared to that of a one component system at the same concentration. As a consequence of this decrease, the gelation concentration is lowered, At higher concentrations a gelling to nongelling transition was observed. In the nongelling regime the colloidal aggregates are kept apart by the impurity clusters, developing a local ordering. For the monomeric type of impurity, at large impurity molar fractions, a nonstructured nongelling phase appears at high enough concentration, in which the colloidal aggregates are kept apart by the sea of mobile impurities that inhibits the formation of a gel. Smaller molar fractions of mobile monomeric impurities strongly affect both the fractal dimension and the kinetics of the aggregating colloid
MH - Mexico|Morelos
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 0
U4 - Physics, Fluids & Plasmas;Physics, Mathematical
U5 - J;Article
AV - English
IS - 1063-651X
UR - ISI:000087575400017
L2 - SELF-SIMILARITY; SCATTERING; DIFFUSION; CRYSTALLIZATION; SIMULATIONS; DEPENDENCE; AEROGELS; NEUTRON; MODEL; PHASE
SO - Physical Review e 2000 ;61(6):6781-6788
82
UI - 16612
AU - AlSunaidi A
AU - Lach-hab M
AU - Gonzalez AE
AU - Blaisten-Barojas E
AD - George Mason Univ, Inst Computat Sci & Informat, Fairfax, VA 22030, USAUniv Maryland, Inst Phys Sci & Technol, College Pk, MD 20742, USAUniv Nacl Autonoma Mexico, Ctr Ciencias Fis, Cuernavaca 62251, Morelos, MexicoAlSunaidi, A, George Mason Univ, Inst Computat Sci & Informat, Fairfax, VA 22030 USA
TI - Cluster-cluster aggregation in binary mixtures
AB - The structure and aggregation kinetics of three-dimensional clusters composed of two different monomeric species at three concentrations are thoroughly investigated by means of extensive, large-scale computer simulations. The aggregating monomers have all the same size and occupy the cells of a cubic lattice,Two;bonding schemes are considered: (a) the binary diffusion-limited cluster-cluster aggregation (BDLCA) in-which only the monomers of different species stick together, and (b) the invading binary diffusion-limited cluster-cluster aggregation (IBDLCA)in which additionally monomers of one of the two species are allowed to bond. In the two schemes, the mixed aggregates display self-similarity with a fractal dimension d(f) that depends on the relative molar fraction of the two species and on concentration. At a given concentrating when this molar fraction is small, df approaches a value close to the reaction-limited cluster-cluster aggregation of one component systems, and when the molar fraction is 0.5, df becomes close to the value of the diffusion-limited cluster-cluster aggregation model. The crossover between these two regimes is due to a time-decreasing reaction probability between colliding particles, particularly at small molar fractions. Several dynamical quantities are studied as a function of time. The number of clusters and the weight-average cluster size display a power-law behavior only at small concentrations. The dynamical exponents are obtained for molar fractions above 0.3 but not at or below 0.2, indicating the presence of a critical transition between a gelling to a nongelling system. The cluster-size distribution function presents scaling for molar fractions larger than 0.2. PACS number(s): 61.43.Hv, 82.70.Dd, 82.70.Gg, 05.10.Ln
MH - Mexico|Morelos
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 5
U4 - Physics, Fluids & Plasmas;Physics, Mathematical
U5 - J;Article
AV - English
IS - 1063-651X
UR - ISI:000084935200073
L2 - COLLOIDAL AGGREGATION; LIMITED AGGREGATION; SELF-SIMILARITY; HETEROCOAGULATION
SO - Physical Review e 2000 ;61(1):550-556
83
UI - 16525
AU - Altamirano MM
AU - Blackburn JM
AU - Aguayo C
AU - Fersht AR
AD - Cambridge Ctr Prot Engn, Cambridge CB2 2QH, EnglandUniv Cambridge, Chem Lab, MRC Ctr, Cambridge CB2 2QH, EnglandNatl Autonomous Univ Mexico, Fac Med, Dept Bioquim, Mexico City 04510, DF, MexicoFersht, AR, Cambridge Ctr Prot Engn, Hills Rd, Cambridge CB2 2QH, England
TI - Directed evolution of new catalytic activity using the alpha/beta-barrel scaffold (Retracted article. See vol 417, pg 468, 2002)
AB - In biological systems, enzymes catalyse the efficient synthesis of complex molecules under benign conditions, but widespread industrial use of these biocatalysts depends crucially on the development of new enzymes with useful catalytic functions. The evolution of enzymes in biological systems often involves the acquisition of new catalytic or binding properties by an existing protein scaffold. Here we mimic this strategy using the most common fold in enzymes, the alpha/beta-barrel, as the scaffold. By combining an existing binding site for structural elements of phosphoribosylanthranilate with a catalytic template required for isomerase activity, we are able to evolve phosphoribosylanthranilate isomerase activity from the scaffold of indole-3-glycerolphosphate synthase, We find that targeting the catalytic template for in vitro mutagenesis and recombination, followed by in vivo selection, results in a new phosphoribosylanthranilate isomerase that has catalytic properties similar to those of the natural enzyme, with an even higher specificity constant. Our demonstration of divergent evolution and the widespread occurrence of the alpha/beta-barrel suggest that this scaffold may be a fold of choice for the directed evolution of new biocatalysts
MH - United Kingdom
MH - Mexico|Distrito Federal
PB - LONDON: MACMILLAN MAGAZINES LTD
RP - NOT IN FILE
U3 - TC 122
U4 - Multidisciplinary Sciences
U5 - J;Article
AV - English
IS - 0028-0836
UR - ISI:000085288200041
L2 - PHOSPHORIBOSYL ANTHRANILATE ISOMERASE; INDOLEGLYCEROL-PHOSPHATE SYNTHASE; IN-VITRO RECOMBINATION; MUCONATE LACTONIZING ENZYME; BETA-SHEET BARRELS; ESCHERICHIA-COLI; MOLECULAR EVOLUTION; BIFUNCTIONAL ENZYME; TRYPTOPHAN BIOSYNTHESIS; MANDELATE RACEMASE
SO - Nature 2000 ;403(6770):617-622
84
UI - 14298
AU - Alvarado E
AU - Torres-Martinez LM
AU - Fuentes AF
AU - Quintana P
AD - IPN, CINVESTAV, Unidad Merida, Merida 97310, Yucatan, VenezuelaUANL, DES, Fac Ciencias Quim, Monterrey, NL, MexicoQuintana, P, IPN, CINVESTAV, Unidad Merida, Km 6 Antigua Carretera Progreso, Merida 97310, Yucatan, Venezuela
TI - Preparation and characterization of MgO powders obtained from different magnesium salts and the mineral dolomite
AB - The characterisation of the physical properties of MgO powders, obtained from three commercial magnesium compounds, MgSO4. 7H(2)O, MgNO3. 6H(2)O and Mg(CH3CO(2))(2). 4H(2)O and the mineral dolomite (natural source from Mexico), synthesised by chemical precipitation, is presented. The decomposition of the precipitated Mg(OH)(2) was analysed by DTA/TGA and the crystallisation process was observed by XRD. The variation of the properties with the nature of the precursors at 960 degreesC was studied: as the crystallite size, density, specific surface area, degree of agglomeration, and the total porosity. The microstructural differences between the MgO agglomerates were examined by SEM, at different temperatures. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Nuevo Leon
MH - Venezuela
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 13
U4 - Chemistry, Inorganic & Nuclear;Crystallography
U5 - J;Article
AV - English
IS - 0277-5387
UR - ISI:000166064800015
L2 - magnesia;dolomite;crystallite size;degree of agglomeration;X-ray diffraction;SEM;EVAPORATIVE DECOMPOSITION
SO - Polyhedron 2000 ;19(22-23):2345-2351
85
UI - 15759
AU - Alvarez F
AU - Villalobos JL
AU - Iliffe TM
AD - Univ Nacl Autonoma Mexico, Inst Biol, Colecc Nacl Crustaceos, Mexico City 04510, DF, MexicoTexas A&M Univ, Dept Marine Biol, Galveston, TX 77553, USAAlvarez, F, Univ Nacl Autonoma Mexico, Inst Biol, Colecc Nacl Crustaceos, Apartado Postal 70-153, Mexico City 04510, DF, Mexico
TI - Naushonia manningi, new species (Decapoda : Thalassinidea : Laomediidae), from Acklins Island, Bahamas
AB - A new species of the rare laomediid genus Naushonia, N. manningi, is described from a cave in Acklins Island. Bahamas. Naushonia manningi represents the seventh species of the genus and the first one to come from a cave. A key to the species of Naushonia is presented
MH - Mexico|Distrito Federal
MH - USA
PB - SAN ANTONIO: CRUSTACEAN SOC
RP - NOT IN FILE
U3 - TC 5
U4 - Marine & Freshwater Biology
U5 - J;Article
AV - English
IS - 0278-0372
UR - ISI:000087883000020
SO - Journal of Crustacean Biology 2000 ;20(2):192-198
86
UI - 14231
AU - Alvarez J
AU - Orlov I
AU - Acho L
AD - Sci Res & Adv Studies Ctr, Elect & Telecommun Dept, Ensenada, Baja California, MexicoUniv Autonoma Baja California, Fac Ingn, Ensenada, Baja California, MexicoAlvarez, J, CICESE Res Ctr, Dept Elect, POB 434944, San Diego, CA 92143 USA
TI - An invariance principle for discontinuous dynamic systems with application to a Coulomb friction oscillator
AB - An invariance principle for a class of ordinary differential equations with discontinuous right-hand side is developed. Based on this principle, asymptotic stability of one-degree-of-freedom mechanical oscillators which Coulomb friction is studied. The system is shown to be asymptotically stabilizable via a static feedback of the position, unlike those systems with no friction, whose stabilization requires a dynamic feedback when the position is the only available measurement. Along with this development, a velocity observer is proposed. Theoretical results of the paper are supported by some numerical simulations which, in addition, carry out a finite-time convergence of the controller and the observer proposed. [S0022-0434(00)00804-2]
MH - Mexico|Baja California
MH - USA
PB - NEW YORK: ASME-AMER SOC MECHANICAL ENG
RP - NOT IN FILE
U3 - TC 17
U4 - Automation & Control Systems;Instruments & Instrumentation
U5 - J;Article
AV - English
IS - 0022-0434
UR - ISI:000167109200017
L2 - FEEDBACK
SO - Journal of Dynamic Systems Measurement and Control-Transactions of the Asme 2000 ;122(4):687-690
87
UI - 16183
AU - Amigo MC
AU - Khamashta MA
AD - Univ Nacl Autonoma Mexico, Dept Rheumatol, Inst Nacl Cardiol Ignacio Chavez, Mexico City 14080, DF, MexicoUnited Med & Dent Sch Guys & St Thomas Hosp, St Thomas Hosp, London SE1 7EH, EnglandUnited Med & Dent Sch Guys & St Thomas Hosp, Guys Hosp, London SE1 9RT, EnglandSt Thomas Hosp, Rayne Inst, Lupus Res Unit, London, EnglandAmigo, MC, Univ Nacl Autonoma Mexico, Dept Rheumatol, Inst Nacl Cardiol Ignacio Chavez, Juan Badiano 1, Mexico City 14080, DF, Mexico
TI - Antiphospholipid (Hughes) syndrome in systemic lupus erythematosus
AB - The antiphospholipid (Hughes) syndrome (APS) was initially described in connection with SLE. It occurs in approximately 30% of patients with SLE. Clinical features and aPL specificities are similar between the primary and secondary forms of APS. The clinical course of the secondary syndrome is independent of the activity and severity of lupus, but the presence of the APS worsens the prognosis of patients with lupus. Treatment of the APS remains empirical and directed at coagulation mechanisms and immune mechanisms because of the limited amount of controlled prospective data
MH - United Kingdom
MH - Mexico|Distrito Federal
PB - PHILADELPHIA: W B SAUNDERS CO
RP - NOT IN FILE
U3 - TC 23
U4 - Rheumatology
U5 - J;Article
AV - English
IS - 0889-857X
UR - ISI:000086361900008
L2 - THROMBOEMBOLIC PULMONARY-HYPERTENSION; LOW-DOSE ASPIRIN; ANTICARDIOLIPIN ANTIBODIES; VENOUS THROMBOSIS; SYNDROME PAPS; DISEASE; ANTICOAGULANT; PREGNANCY; CRITERIA; HEPARIN
SO - Rheumatic Disease Clinics of North America 2000 ;26(2):331-+
88
UI - 16485
AU - Amigo V
AU - Ortiz JL
AU - Salvador MD
AD - UPV, Dept Ingn Mecan & Mat, Valencia 46022, SpainITESM, Dept Ingn Mecan & Ind, Santiago De Queretaro 76130, MexicoAmigo, V, UPV, Dept Ingn Mecan & Mat, Camino Vera S-N, Valencia 46022, Spain
TI - Microstructure and mechanical behavior of 6061Al reinforced with silicon nitride particles, processed by powder metallurgy
MH - Mexico|Queretaro
MH - Spain
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 12
U4 - Nanoscience & Nanotechnology;Materials Science, Multidisciplinary;Metallurgy & Metallurgical Engineering
U5 - J;Article
AV - English
IS - 1359-6462
UR - ISI:000085431900011
L2 - extrusion;powder consolidation;aluminium;aging;MATRIX COMPOSITES; AGING BEHAVIOR; PARTICULATE COMPOSITES; TENSILE PROPERTIES; SIC/AL COMPOSITES; TEMPERATURE; PRECIPITATION; ALUMINUM; SIZE
SO - Scripta Materialia 2000 ;42(4):383-388
89
UI - 13029
AU - Amorin H
AU - Portelles J
AU - Guerrero F
AU - Fundora A
AU - Siqueiros-Beltrones JM
AD - UNAM, Ctr Ciencias Mat Condensada, Ensenada 22800, Baja California, MexicoUniv La Habana, Fac Fis, Inst Mat & React, Havana 10400, CubaUniv Oriente, Fac Ciencias Nat, Santiago De Cuba 90500, CubaSiqueiros-Beltrones, JM, UNAM, Ctr Ciencias Mat Condensada, Apartado Postal 2681, Ensenada 22800, Baja California, Mexico
TI - Diffuse phase transition in the (La0.03Sr0.255Ba0.7)(Nb2-yTiy)O-6.y/2 ferroelectric ceramic system
AB - The effect of the titanium cation as a doping element in the diffuse phase transition of the (Sr0.255La0.03Ba0.7)(Nb2-yTiy)O6-y/2 ferroelectric ceramic system is studied. Far from the transition temperature, a Curie-Weiss behavior of the dielectric permittivity with temperature is observed with strongly broadened curves in all cases, however, a non Curie-Weiss behavior above the transition temperature is observed. The diffuseness coefficient (delta) was calculated using Isupov's relation and by a more realistic model assuming a Gaussian distribution for the transition temperatures, in a temperature interval around the maximum permittivity temperature. The conditions under which each expression can be used are discussed
MH - Cuba
MH - Mexico|Baja California
PB - PHILADELPHIA: GORDON BREACH PUBLISHING, TAYLOR & FRANCIS GROUP
RP - NOT IN FILE
U3 - TC 2
U4 - Materials Science, Multidisciplinary;Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0015-0193
UR - ISI:000170518300009
L2 - ferroelectric ceramics;diffuse phase transition;modified Sr1-xBaxNb2O6 system;STRONTIUM BARIUM NIOBATE; GLASSY POLARIZATION; BEHAVIOR
SO - Ferroelectrics 2000 ;248(1-4):97-106
90
UI - 15354
AU - Amorin H
AU - Portelles J
AU - Guerrero F
AU - Fundora A
AU - Martinez E
AU - Siqueiros JM
AD - Univ Havana, Fac Fis, Inst Mat & Reactivos, Havana 10400, CubaUNAM, Ctr Ciencias Mat Condensada, Ensenada 22800, Baja California, MexicoUniv Oriente, Fac Ciencias Nat, Santiago 90500, CubaUNAM, Ctr Ciencias Mat Condensada, Ensenada 22800, Baja California, MexicoAmorin, H, Univ Havana, Fac Fis, Inst Mat & Reactivos, San Lazaro & L Vedado, Havana 10400, Cuba
TI - Formation of the La0.03Sr0.255Ba0.7Nb2-yTiyO6-y/2 ferroelectric ceramic system
AB - The study of the formation of the Sr0.255La0.03Ba0.7Nb2 - yTiyO6 - y/2 ferroelectric ceramic system and the influence of the sintering conditions and titanium concentration on the densification process is reported. A single-phase compound is observed for low titanium content (y less than or equal to 0.1) in the XRD spectra, being isostructural with the tetragonal tungsten bronze SBN phase. For high titanium concentrations (y > 0.1) the XRD patterns show, besides the tetragonal phase reflections, several small peaks evidencing an additional phase in the compound. This second phase was identified as isostructural to hexagonal Ba6Nb9Ti7O42. The grain size shows a linear increase with titanium content in the region of monophasic compositions and a possible liquid phase aided sintering process is analyzed. (C) 2000 Kluwer Academic Publishers
MH - Cuba
MH - Mexico|Baja California
PB - DORDRECHT: KLUWER ACADEMIC PUBL
RP - NOT IN FILE
U3 - TC 2
U4 - Materials Science, Multidisciplinary
U5 - J;Article
AV - English
IS - 0022-2461
UR - ISI:000088984000017
L2 - STRONTIUM BARIUM NIOBATE; DIELECTRIC-PROPERTIES; DETECTORS; CRYSTALS
SO - Journal of Materials Science 2000 ;35(18):4607-4613
91
UI - 16519
AU - Amorin H
AU - Portelles J
AU - Guerrero F
AU - Perez J
AU - Siqueiros JM
AD - Univ La Habana, Fac Fis, IMRE, Havana 10400, CubaUNAM, Ctr Ciencias Mat Condensada, Ensenada 22800, Baja California, MexicoUniv Oriente, Fac Ciencias Nat, Santiago De Cuba 90500, CubaAmorin, H, Univ La Habana, Fac Fis, IMRE, Havana 10400, Cuba
TI - Dielectric hysteresis and pyroelectricity in the La0.03Sr0.255Ba0.7Nb2-yTiyO(6-y)/2 ferroelectric ceramic system
AB - The dielectric hysteresis and pyroelectric properties of the La0.03Sr0.255Ba0.7Nb2-yTiyO(6-y)/2 (LSBNT) ceramic system were studied for different Nb/Ti concentrations. For dielectric hysteresis measurements at room temperature, the remanent polarization increases and the: coercive field decreases with titanium concentration for an applied electric field of 20 kV/cm. The thermally stimulated current measurements show the pyroelectric peak for all compositions while a second smaller peak at higher temperature, possibly associated with induced vacancy-impurity dipoles, is also observed in all cases. The second peak contribution was mathematically eliminated to determine the remanent polarization and pyroelectric coefficient, both associated only with permanent ferroelectric dipoles. In this case, the remanent polarization decreased with the rise in titanium concentration. The La0.03Sr0.255Ba0.7Nb1.95Ti0.05O5.975 sample, in particular, has excellent pyroelectric response, making this material very suitable for pyroelectricity-derived applications. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Cuba
MH - Mexico|Baja California
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 6
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0038-1098
UR - ISI:000085275400009
L2 - ferroelectronics;chemical synthesis;dielectric response;MODIFIED SR0.5BA0.5NB2O6; DETECTORS; CRYSTALS
SO - Solid State Communications 2000 ;113(10):581-585
92
UI - 14964
AU - Anderson ARA
AU - Chaplain MAJ
AU - Garcia-Reimbert C
AU - Vargas CA
AD - Univ Dundee, Dept Math, Dundee DD1 4HN, ScotlandUniv Nacl Autonoma Mexico, IIMAS, FENOMEC, Mexico City 01000, DF, MexicoUniv Nacl Autonoma Mexico, IIMAS, Dept Matemat & Mecan, Mexico City 01000, DF, MexicoAnderson, ARA, Univ Dundee, Dept Math, Dundee DD1 4HN, Scotland
TI - A gradient-driven mathematical model of antiangiogenesis
AB - In this paper, we present a mathematical model describing the angiogenic response of endothelial cells to a secondary tumour. It has been observed experimentally that while the primary tumour remains in situ, any secondary tumours that may be present elsewhere in the host can go undetected, whereas removal of the primary tumour often leads to the sudden appearance of these hitherto undetected metastases-so-called occult metastases. In this paper, a possible explanation for this suppression of secondary tumours by the primary tumour is given in terms of the presumed migratory response of endothelial cells in the neighbourhood of the secondary tumour. Our model assumes that the endothelial cells respond chemotactically to two opposing chemical gradients: a gradient of tumour angiogenic factor, set up by the secretion of angiogenic cytokines from the secondary tumour; and a gradient of angiostatin, set up in the tissue surrounding any nearby vessels. The angiostatin arrives there through the blood system (circulation), having been originally secreted by the primary tumour. This gradient-driven endothelial cell migration therefore provides a possible explanation of how secondary tumours (occult metastases) can remain undetected in the presence of the primary tumour yet suddenly appear upon surgical removal of the primary tumour. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Mexico|Distrito Federal
MH - United Kingdom
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 3
U4 - Computer Science, Interdisciplinary Applications;Computer Science, Software Engineering;Mathematics, Applied
U5 - J;Article
AV - English
IS - 0895-7177
UR - ISI:000165051800006
L2 - antiangiogenesis;angiostatin;endothelial cells;tumour angiogenic factors;chemotaxis;TUMOR-RELATED ANGIOGENESIS; ENDOTHELIAL-CELLS; METASTASIS; GROWTH; NEOVASCULARIZATION; PROLIFERATION; ANGIOSTATIN; MECHANISMS; INHIBITOR; INVASION
SO - Mathematical and Computer Modelling 2000 ;32(10):1141-1152
93
UI - 16260
AU - Andrade E
AU - Garcia VM
AU - Nair PK
AU - Nair MTS
AU - Zavala EP
AU - Huerta L
AU - Rocha MF
AD - Univ Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoUniv Autonoma Zacatecas, Fac Ciencias Quim, Zacatecas 98600, GuadeloupeUniv Nacl Autonoma Mexico, Inst Politecn Nacl, Escuela Super Ingn Mecan Elect, Mexico City 07738, DF, MexicoAndrade, E, Univ Nacl Autonoma Mexico, Inst Fis, Apartado Postal 20-364, Mexico City 01000, DF, Mexico
TI - Ion beam analysis of copper selenide thin films prepared by chemical bath deposition
AB - Analyses of Rutherford back scattered (RBS) He-4(+)-particle spectra of copper selenide thin films deposited on glass slides by chemical bath were carried out to determine the changes brought about in the thin him by annealing processes. The atomic density per unit area and composition of the films were obtained from these measurements. This analysis shows that annealing in a nitrogen atmosphere at 400 degrees C leads to the conversion of CuxSe thin film to Cu2Se. Results of X-ray diffraction, optical, and electrical characteristics on the films are presented to supplement the RBS results. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Guadeloupe
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 2
U4 - Instruments & Instrumentation;Nuclear Science & Technology;Physics, Atomic, Molecular & Chemical;Physics, Nuclear
U5 - J;Article
AV - English
IS - 0168-583X
UR - ISI:000086204100120
L2 - IBA techniques;chemical composition;X-ray diffractometry;thin film growth;chemical deposition
SO - Nuclear Instruments & Methods in Physics Research Section B-Beam Interactions with Materials and Atoms 2000 ;161():635-640
94
UI - 15941
AU - Andrade L
AU - Caraveo-Anduaga JJ
AU - Berglund P
AU - Bijl R
AU - Kessler RC
AU - Demler O
AU - Walters E
AU - Kylyc C
AU - Offord D
AU - Ustun TB
AU - Wittchen HU
AD - Harvard Univ, Sch Med, Dept Hlth Care Policy, Boston, MA 02115, USAMexican Inst Psychiat, Mexico City, DF, MexicoUniv Michigan, Ann Arbor, MI 48109, USANetherlands Inst Mental Hlth & Addict, Utrecht, NetherlandsHacettepe Univ, Sch Med, Ankara, TurkeyChedoke McMaster Hosp, Hamilton, ON, CanadaWHO, ACE, CH-1211 Geneva, SwitzerlandMax Planck Inst Psychiat, D-8000 Munich, GermanyUniv Sao Paulo, Sao Paulo, BrazilKessler, RC, Harvard Univ, Sch Med, Dept Hlth Care Policy, 180 Longwood Ave, Boston, MA 02115 USA
TI - Cross-national comparisons of the prevalences and correlates of mental disorders
AB - The International Consortium in Psychiatric Epidemiology (ICPE) was established in 1998 by WHO to carry out cross-national comparative studies of the prevalences and correlates of mental disorders. This article describes the findings of ICPE surveys in seven countries in North America (Canada and USA), Latin America (Brazil and Mexico), and Europe (Germany, Netherlands, and Turkey), using a version of the WHO Composite International Diagnostic Interview (CIDI) to generate diagnoses. The results are reported using DSM-III-R and DSM-IV criteria without diagnostic hierarchy rules for mental disorders and with hierarchy rules for substance-use disorders. Prevalence estimates varied widely - from >40% lifetime prevalence of any mental disorder in Netherlands and the USA to levels of 12% in Turkey and 20% in Mexico. Comparisons of lifetime versus recent prevalence estimates show that menta I disorders were often ch ron ic, although chronicity was consistently higher for anxiety disorders than for mood or substance-use disorders. Retrospective reports suggest that mental disorders typically had early ages of onset, with estimated medians of 15 years for anxiety disorders, 26 years for mood disorders, and 21 years for substance-use disorders. All three classes of disorder were positively related to a number of socioeconomic measures of disadvantage (such as low income and education, unemployed, unmarried). Analysis of retrospective age-of-onset reports suggest that lifetime prevalences had increased in recent cohorts, but the increase was less for anxiety disorders than for mood or substance-use disorders. Delays in seeking professional treatment were widespread, especially among early-onset cases, and only a minority of people with prevailing disorders received any treatment. Mental disorders are among the most burdensome of all classes of disease because of their high prevalence and chronicity, early age of onset, and resulting serious impairment. There is a need for demonstration projects of early outreach and intervention programmes for people with early-onset mental disorders, as well as quality assurance programmes to look into the widespread problem of inadequate treatment
MH - Brazil
MH - Canada
MH - Germany
MH - USA
MH - Mexico|Distrito Federal
MH - Netherlands
MH - Switzerland
MH - Turkey
PB - GENEVA 27: WORLD HEALTH ORGANIZATION
RP - NOT IN FILE
U3 - TC 106
U4 - Public, Environmental & Occupational Health
U5 - J;Article
AV - English
IS - 0042-9686
UR - ISI:000087313700003
L2 - mental disorders, epidemiology;psychiatric status rating scales;cross-cultural comparison;cross-sectional studies;North America;Latin America;Europe;CHRISTCHURCH PSYCHIATRIC EPIDEMIOLOGY; INTERNATIONAL DIAGNOSTIC INTERVIEW; UNITED-STATES; SOCIAL-CONSEQUENCES; LIFETIME PREVALENCE; COMORBIDITY-SURVEY; TREATMENT CONTACT; MAJOR DEPRESSION; MEDICAL OUTCOMES; HEALTH
SO - Bulletin of the World Health Organization 2000 ;78(4):413-426
95
UI - 14978
AU - Anglada G
AU - Rodriguez LF
AU - Torrelles JM
AD - CSIC, Inst Astrofis Andalucia, E-18008 Granada, SpainUniv Nacl Autonoma Mexico, Inst Astron, Morelia 58089, Michoacan, MexicoCSIC, IEEC, E-08034 Barcelona, SpainCSIC, Inst Ciencias Espacio, E-08034 Barcelona, SpainAnglada, G, CSIC, Inst Astrofis Andalucia, Camino Bajo Huetor 24, E-18008 Granada, Spain
TI - Discovery of a subarcsecond radio binary associated with the SVS 13 star in the HH 7-11 region
AB - We report the discovery of a double radio continuum source (VLA 4A and 4B) associated with the optically visible star SVS 13. The two components of the radio source are separated by 0".3, corresponding to a projected separation of 65 AU for a distance of 220 pc. We propose that the radio sources trace the components of a binary system. The observed separation implies a lower limit of similar to 135 yr for the orbital period, for a binary system with a total mass of 2 M-.. We suggest that, as in other pre-main-sequence binaries, the two components of the system could be in different evolutionary stages and/or suffer from different extinction, with the more extincted object being associated with the previously reported millimeter source, while the other component would correspond to the visible star SVS 13. Since an increase in the optical/near-infrared brightness of the SVS 13 star was observed around 1990, we speculate that such flux variations could be due to the reappearance of the optical component previously occulted by the circumstellar envelope/disk of dust associated with the millimeter component. The observed separation implies a radius of similar to 60 AU for the presumed dust envelope and suggests an orbital period of similar to 1700 yr and a duration of the occultation of similar to 185 yr. We expect that other subarcsecond binary systems, which remain unresolved, could present an anomalous behavior that may be explained by assuming the presence of a binary system whose components are in different evolutionary stages and/or suffer from different extinction
MH - Mexico|Michoacan
MH - Spain
PB - CHICAGO: UNIV CHICAGO PRESS
RP - NOT IN FILE
U3 - TC 11
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-637X
UR - ISI:000165095700012
L2 - ISM : individual (HH 7-11);ISM : jets and outflows;radio continuum : ISM;stars : formation;stars : individual (SVS 13);HERBIG-HARO OBJECTS; T-TAURI STARS; INFRARED COMPANION; EXCITING SOURCE; NGC-1333; OUTBURST; SSV-13; HH7-11; DISKS; FLOW
SO - Astrophysical Journal 2000 ;542(2):L123-L126
96
UI - 16662
AU - Angulo Y
AU - Olamendi-Portugal T
AU - Possani LD
AU - Lomonte B
AD - Univ Costa Rica, Fac Microbiol, Inst Clodomiro Picado, Escuela Med, San Jose, Costa RicaUniv Costa Rica, Escuela Med, Dept Bioquim, San Jose, Costa RicaNatl Autonomous Univ Mexico, Inst Biotecnol, Dept Mol Recognit & Struct Biol, Cuernavaca, Morelos, MexicoLomonte, B, Univ Costa Rica, Fac Microbiol, Inst Clodomiro Picado, Escuela Med, San Jose, Costa Rica
TI - Isolation and characterization of myotoxin II from Atropoides (Bothrops) nummifer snake venom, a new Lys49 phospholipase A(2) homologue
AB - Myotoxic phospholipases A(2) Of class II are commonly found in: the venoms of crotalid snakes. As an approach to understanding their structure-activity relationship, diverse natural variants: have been characterized biochemically and pharmacologically. This study describes a new myotoxic phospholipase Az homologue, isolated from the venom of Atropoides (Bothrops) nummifer from Costa Rica, A. nummifer myotoxin II is a basic protein, with an apparent subunit molecular mass of 16 kDa, which migrates as a dimer in sodium dodecylsulfate-polyacrylamide gel electrophoresis under nonreducing conditions. It is strongly recognized by antibodies generated against Bothrops asper:myotoxin II, by enzyme-immunoassay. The toxin induces rapid myonecrosis upon intramuscular injection in mice (evidenced by an early increase in plasma creatine kinase activity), and significant edema in the footpad assay. It also displays cytolytic activity upon cultured murine endothelial cells, The toxin (up to 50 mu g) has no detectable phospholipase A(2) activity on egg yolk phospholipids, and does not show an anticoagulant effect on sheep platelet-poor plasma in vitro. N-terminal sequence determination (53 amino acid residues) demonstrated that A. nummifer myotoxin II is a new Lys49 variant of the family of myotoxic, class II phospholipases A(2). Sequence comparison with other phospholipases A(2) revealed Asn53 as a novel substitution. In addition, this myotoxin is the first Lys49 variant presenting Asn in its N-terminus. Consequently, these findings suggest that neither Ser1 or Lys53, usually found in this family of proteins, are essential amino acid residues for their myotoxic, cytolytic, or edema-inducing effects. (C) 1999 Elsevier Science Ltd. All rights reserved
MH - Costa Rica
MH - Mexico|Morelos
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 16
U4 - Biochemistry & Molecular Biology;Cell Biology
U5 - J;Article
AV - English
IS - 1357-2725
UR - ISI:000084663800006
L2 - snake venom;myotoxin;phospholipase A(2);Atropoides nummifer;Bothrops;AMINO-ACID-SEQUENCE; LYSINE-49 PHOSPHOLIPASE-A(2); ASPER TERCIOPELO; COSTA-RICA; IDENTIFICATION; CALCIUM; PROTEIN; CLONING; BINDING; REGION
SO - International Journal of Biochemistry & Cell Biology 2000 ;32(1):63-71
97
UI - 16441
AU - Anikiev VV
AU - Dudarev OV
AU - Said MA
AU - Botsul AI
AU - Utkin IV
AU - Shumilin EN
AD - Russian Natl Ecol Safety Comm, Moscow 101000, RussiaPacific Oceanol Inst, Vladivostok 690041, RussiaEgyptian Acad Sci, Oceanog & Fishery Natl Inst, Alexandria, EgyptLa Paz Marine Ctr, La Paz 23000, MexicoAnikiev, VV, Russian Natl Ecol Safety Comm, Ul Lubyanka 10, Moscow 101000, Russia
TI - Natural and anthropogenic factors in the lateral distribution of the particulate material and chemical elements in water of the Nile river foredelta and adjacent area of the Mediterranean Sea
MH - Egypt
MH - Mexico|Baja California Sur
MH - Russia
PB - MOSCOW: ROSSIISKAYA AKADEMIYA NAUK
RP - NOT IN FILE
U3 - TC 0
U4 - Geochemistry & Geophysics
U5 - J;Article
AV - Russian
IS - 0016-7525
UR - ISI:000085353400007
L2 - EGYPTIAN COAST; HEAVY-METALS; BEHAVIOR; ESTUARY; FE; MN; ZN; CU
SO - Geokhimiya 2000 ;(1):78-91
98
UI - 15324
AU - Aposhian HV
AU - Zheng BS
AU - Aposhian MM
AU - Le XC
AU - Cebrian ME
AU - Cullen W
AU - Zakharyan RA
AU - Ma HS
AU - Dart RC
AU - Cheng Z
AU - Andrewes P
AU - Yip L
AU - O'Malley GF
AU - Maiorino RM
AU - Van Voorhies W
AU - Healy SM
AU - Titcomb A
AD - Univ Arizona, Dept Mol & Cellular Biol, Tucson, AZ 85721, USAAcad Sinica, Inst Geochem, State Key Lab Environm Geochem, Guiyang 550002, Guizhou, Peoples R ChinaUniv Alberta, Fac Med & Dent, Dept Publ Hlth Sci, Edmonton, AB T6G 2G3, CanadaInst Politecn Nacl, CINVESTAV, Secc Toxicol Ambientale, Mexico City 07000, DF, MexicoUniv British Columbia, Dept Chem, Vancouver, BC V6T 1Z1, CanadaRocky Mt Poison & Drug Control Ctr, Denver, CO 80220, USAW China Univ Med Sci, Dept Epidemiol, Shenyang 110001, Liaoning, Peoples R ChinaAposhian, HV, Univ Arizona, Dept Mol & Cellular Biol, LSS Bldg,Room 444,POB 210106, Tucson, AZ 85721 USA
TI - DMPS - Arsenic Challenge Test II. Modulation of arsenic species, including monomethylarsonous acid (MMA(III)), excreted in human urine
AB - The administration of sodium 2,3-dimercapto-1-propane sulfonate (DMPS) to humans chronically exposed to inorganic arsenic in their drinking water resulted in the increased urinary excretion of arsenic, the appearance and identification of monomethylarsonous acid (MMA(III)) in their urine, and a large decrease in the concentration and percentage of urinary dimethylarsinic acid (DMA). This is the first time that MMA(III) has been detected in the urine. In vitro biochemical experiments were then designed and performed to understand the urinary appearance of MMA(III) and decrease of DMA. The DMPS-MMA(III) complex was not active as a substrate for the MMA(III) methyltransferase. The experimental results support the hypothesis that DMPS competes with endogenous ligands for MMA(III), forming a DMPS-MMA complex that is readily excreted in the urine and points out the need for studying the biochemical toxicology of MMA(III). It should be emphasized that MMA(III) was excreted in the urine only after DMPS administration. The results of these studies raise many questions about the potential central role of MMA(III) in the toxicity of inorganic arsenic and to the potential involvement of MMA(III) in the Little-understood etiology of hyperkeratosis, hyperpigmentation, and cancer that can result from chronic inorganic arsenic exposure, (C) 2000 Academic Press
MH - USA
MH - Canada
MH - Mexico|Distrito Federal
MH - Peoples R China
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 61
U4 - Pharmacology & Pharmacy;Toxicology
U5 - J;Article
AV - English
IS - 0041-008X
UR - ISI:000089000900007
L2 - MMA(III);monomethylarsonous acid;arsenic biotransformation;DMPS;arsenic;ENZYMATIC METHYLATION; CHELATING-AGENTS; DRINKING-WATER; RABBIT LIVER; WELL-WATER; 2,3-DIMERCAPTOPROPANE-1-SULFONATE; METHYLTRANSFERASE; CARCINOGENESIS; SPECIATION; METABOLISM
SO - Toxicology and Applied Pharmacology 2000 ;165(1):74-83
99
UI - 15415
AU - Aposhian HV
AU - Gurzau ES
AU - Le XC
AU - Gurzau A
AU - Healy SM
AU - Lu XF
AU - Ma MS
AU - Yip L
AU - Zakharyan RA
AU - Maiorino RM
AU - Dart RC
AU - Tircus MG
AU - Gonzalez-Ramirez D
AU - Morgan DL
AU - Avram D
AU - Aposhian MM
AD - Univ Arizona, Dept Mol & Cellular Biol, Tucson, AZ 85721, USACtr Environm Hlth, Cluj Napoca 3400, RomaniaUniv Alberta, Fac Med & Dent, Dept Publ Hlth Sci, Edmonton, AB T6G 2G3, CanadaRocky Mt Poison & Drug Control Ctr, Denver, CO 80220, USAState Sanitary Inspect Arad, Arad 2900, RomaniaInst Mexicano Seguro Social, Unidad Invest Biomed Noreste, Dept Farmacol, Monterrey 64720, Nuevo Leon, MexicoNIEHS, Toxicol Lab, Res Triangle Pk, NC 27709, USAAposhian, HV, Univ Arizona, Dept Mol & Cellular Biol, Life Sci S Bldg,Rm 444,POB 210106, Tucson, AZ 85721 USA
TI - Occurrence of monomethylarsonous acid in urine of humans exposed to inorganic arsenic
AB - Monomethylarsonous acid (MMA(III)) has been detected for the first time in the urine of some humans exposed to inorganic arsenic in their drinking water. Our experiments have dealt with subjects in Romania who have been exposed to 2.8, 29, 84, or 161 mu g of As/L in their drinking water. In the latter two groups, MMA(III) was 11 and 7% of the urinary arsenic while the monomethylarsonic acid (MMA(V)) was 14 and 13%, respectively. Of our 58 subjects, 17% had MMA(III) in their urine. MMA(III) was not found in urine of any members of the group with the lowest level of As exposure. If the lowest-level As exposure group is excluded, 23% of our subjects had MMA(III) in their urine. Our results indicate that (a) future studies concerning urinary arsenic profiles of arsenic-exposed humans must determine MMA(III) concentrations, (b) previous studies of urinary profiles dealing with humans exposed to arsenic need to be re-examined and re-evaluated, and (c) since MMA(III) is more toxic than inorganic arsenite, a re-examination is needed of the two hypotheses which hold that methylation is a detoxication process for inorganic arsenite and that inorganic arsenite is the major cause of the toxicity and carcinogenicity of inorganic arsenic
MH - USA
MH - Canada
MH - Mexico|Nuevo Leon
MH - Romania
PB - WASHINGTON: AMER CHEMICAL SOC
RP - NOT IN FILE
U3 - TC 119
U4 - Chemistry, Medicinal;Chemistry, Multidisciplinary;Toxicology
U5 - J;Article
AV - English
IS - 0893-228X
UR - ISI:000088951400002
L2 - ENZYMATIC METHYLATION; RABBIT LIVER; WEST-BENGAL; METHYLTRANSFERASE; WATER; TOXICITY
SO - Chemical Research in Toxicology 2000 ;13(8):693-697
100
UI - 15089
AU - Arakeri JH
AU - Avila FE
AU - Dada JM
AU - Tovar RO
AD - Indian Inst Sci, Dept Mech Engn, Bangalore 560012, Karnataka, IndiaUNAM, Temixco, Ctr Invest Energia, Mexico City, DF, MexicoArakeri, JH, Indian Inst Sci, Dept Mech Engn, Bangalore 560012, Karnataka, India
TI - Convection in a long vertical tube due to unstable stratification - A new type of turbulent flow?
AB - We present experimental results of free convection in a vertical tube due to an unstable density difference imposed between the two (open) ends of the tube. Two tanks of fluids connect the two ends of the tube with the top-tank fluid heavier than the bottom-tank fluid. We use salt mixed with water to create the density difference. The convection in the tube is in the form of relatively heavier fluid going down and lighter fluid going up simultaneously; the mean flow at any cross section of the tube is zero. Depending on the Rayleigh number we observe different types of flow, with turbulent flow being observed at the higher Rayleigh numbers. We believe this is a new type of turbulent flow-a nearly homogeneous, buoyancy-driven flow with zero mean shear
MH - India
MH - Mexico|Distrito Federal
PB - BANGALORE: CURRENT SCIENCE ASSN
RP - NOT IN FILE
U3 - TC 1
U4 - Multidisciplinary Sciences
U5 - J;Article
AV - English
IS - 0011-3891
UR - ISI:000089776800030
L2 - INSTABILITY
SO - Current Science 2000 ;79(6):859-866
101
UI - 16581
AU - Aramburo C
AU - Luna M
AU - Carranza M
AU - Reyes M
AU - Martinez-Coria H
AU - Scanes CG
AD - Univ Nacl Autonoma Mexico, Ctr Neurobiol, Queretaro 76001, Qro, MexicoRutgers State Univ, Dept Anim Sci, New Brunswick, NJ 08903, USAAramburo, C, Univ Nacl Autonoma Mexico, Ctr Neurobiol, Campus UNAM UAQ Juriquilla,Apdo Postal 1-1141, Queretaro 76001, Qro, Mexico
TI - Growth hormone size variants: Changes in the pituitary during development of the chicken
AB - There is considerable evidence for the existence of structural variants of growth hormone (GH). The chicken is a useful model for investigating GH heterogeneity as both size and charge immunoreactive-(ir) variants have been observed in the pituitary and plasma. The present study examined the size distribution of ir-GH in the pituitary gland of chicken, from late embryogenesis through adulthood. Pituitaries were homogenized in the presence of protease inhibitor, and the GH size variants were separated by SDS-PAGE, transferred by Western blotting, immunostained with a specific antiserum to chicken GH, and quantitated by chemiluminescence followed by laser densitometry (chemiluminescent assay). Under nonreducing conditions Ir-GH bands of 15, 22, 25, 44, 50, 66, 80, 98, 105 and >110 kDa were observed. Both the relative proportion of the GH sire variants and the total pituitary content varied with developmental stage and age. The proportion of the 15-kDa fragment was greatest in the embryonic stage, and then it decreased. The proportion of the monomeric 22-kDa form was lowest at 18 days of embryogenesis (dE) and highest at 20 dE. In contrast, the high MW forms (greater than or equal to 66 kDa) were lowest in embryos, and they increased (P < 0.05) after hatching. The 22-, 44-, 66-, and 80-kDa forms were assayed for activity by radio-receptor assay following isolation by semipreparative SDS-PAGE. Only the 22-kDa GH variant showed radioreceptor activity. Under reducing conditions for SDS-PAGE, ir-GH bands of 13, 15, 18, 23, 26, 36, 39, 44, 48, 59 and 72 kDa were oberved, but most of the high MW form disappeared. There was a concomitant increase in the proportion of the monomeric band and of several submonomeric forms. The present data indicate that the expression, processing, and/or release of some if not all size variants are under some differential control during growth and development of the chicken
MH - Mexico|Queretaro
MH - USA
PB - MALDEN: BLACKWELL SCIENCE INC
RP - NOT IN FILE
U3 - TC 21
U4 - Medicine, Research & Experimental
U5 - J;Article
AV - English
IS - 0037-9727
UR - ISI:000084988300009
L2 - CGH CHARGE VARIANTS; BIOLOGICAL CHARACTERIZATION; IMMUNOLOGICAL PROPERTIES; NONGLYCOSYLATED FORMS; PROLACTIN; HETEROGENEITY; ISOFORMS; PROTEINS; ONTOGENY; RAT
SO - Proceedings of the Society for Experimental Biology and Medicine 2000 ;223(1):67-74
102
UI - 15707
AU - Aranda JI
AU - Martinez R
AU - Sampayo OA
AD - Univ Michoacana San Nicolas de Hidalgo, Escuela Ciencias Fidicomatemat, Morelia, Michoacan, MexicoUniv Nacl, Dept Fis, Bogota, ColombiaUniv Mar del Plata, Dept Fis, RA-7600 Mar Del Plata, ArgentinaAranda, JI, Univ Michoacana San Nicolas de Hidalgo, Escuela Ciencias Fidicomatemat, Morelia, Michoacan, Mexico
TI - Limits on excited tau lepton masses from leptonic tau decays
AB - We study the effects induced by excited leptons on the leptonic tau decay at the one loop level. Using a general effective Lagrangian approach to describe the couplings of the excited leptons, we compute their contributions to the leptonic decays and use the current experimental values of the branching ratios to put limits on the mass of excited states and the substructure scale
MH - Argentina
MH - Colombia
MH - Mexico|Michoacan
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 2
U4 - Astronomy & Astrophysics;Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 0556-2821
UR - ISI:000087954100016
L2 - ROOT-S=161 GEV; COMPOSITENESS; PHYSICS; SEARCH; MOMENT
SO - Physical Review D 2000 ;6201(1):
103
UI - 15940
AU - Arce H
AU - Xu AX
AU - Gonzalez H
AU - Guevara MR
AD - Natl Autonomous Univ Mexico, Fac Ciencias, Dept Fis, Mexico City 04510, DF, MexicoMcGill Univ, Dept Physiol, Montreal, PQ H3G 1Y6, CanadaMcGill Univ, Ctr Nonlinear Dynam Physiol & Med, Montreal, PQ H3G 1Y6, CanadaArce, H, Natl Autonomous Univ Mexico, Fac Ciencias, Dept Fis, Apartado Postal 70-542, Mexico City 04510, DF, Mexico
TI - Alternans and higher-order rhythms in an ionic model of a sheet of ischemic ventricular muscle
AB - Life-threatening arrhythmias such as ventricular tachycardia and fibrillation often occur during acute myocardial ischemia. During the first few minutes following coronary occlusion, there is a gradual rise in the extracellular concentration of potassium ions ([K+](0)) within ischemic tissue. This elevation of [K+](0) is one of the main causes of the electrophysiological changes produced by ischemia, and has been implicated in inducing arrhythmias. We investigate an ionic model of a 3 cmx3 cm sheet of normal ventricular myocardium containing an ischemic zone, simulated by elevating [K+](0) within a centrally-placed 1 cmx1 cm area of the sheet. As [K+](0) is gradually raised within the ischemic zone from the normal value of 5.4 mM, conduction first slows within the ischemic zone and then, at higher [K+](0), an arc of block develops within that area. The area distal to the arc of block is activated in a delayed fashion by a retrogradely moving wavefront originating from the distal edge of the ischemic zone. With a further increase in [K+](0), the point eventually comes where a very small increase in [K+](0) (0.01 mM) results in the abrupt transition from a global period-1 rhythm to a global period-2 rhythm in the sheet. In the peripheral part of the ischemic zone and in the normal area surrounding it, there is an alternation of action potential duration, producing a 2:2 response. Within the core of the ischemic zone, there is an alternation between an action potential and a maintained small-amplitude response (similar to 30 mV in height). With a further increase of [K+](0), the maintained small-amplitude response turns into a decrementing subthreshold response, so that there is 2:1 block in the central part of the ischemic zone. A still further increase of [K+](0) leads to a transition in the sheet from a global period-2 to a period-4 rhythm, and then to period-6 and period-8 rhythms, and finally to a complete block of propagation within the ischemic core. When the size of the sheet is increased to 4 cmx4 cm (with a 2 cmx2 cm ischemic area), one observes essentially the same sequence of rhythms, except that the period-6 rhythm is not seen. Very similar sequences of rhythms are seen as [K+](0) is increased in the central region (1 or 2 cm long) of a thin strand of tissue (3 or 4 cm long) in which propagation is essentially one-dimensional and in which retrograde propagation does not occur. While reentrant rhythms resembling tachycardia and fibrillation were not encountered in the above simulations, well-known precursors to such rhythms (e.g., delayed activation, arcs of block, two-component upstrokes, retrograde activation, nascent spiral tips, alternans) were seen. We outline how additional modifications to the ischemic model might result in the emergence of reentrant rhythms following alternans. (C) 2000 American Institute of Physics. [S1054-1500(00)00102-6]
MH - Canada
MH - Mexico|Distrito Federal
PB - MELVILLE: AMER INST PHYSICS
RP - NOT IN FILE
U3 - TC 18
U4 - Mathematics, Applied;Physics, Mathematical
U5 - J;Review
AV - English
IS - 1054-1500
UR - ISI:000087346300014
L2 - ACUTE MYOCARDIAL-ISCHEMIA; ACTION-POTENTIAL DURATION; T-WAVE ALTERNANS; PERIOD-DOUBLING BIFURCATIONS; ACUTE CORONARY-OCCLUSION; ACUTE REGIONAL ISCHEMIA; CARDIAC PURKINJE-FIBERS; PERFUSED PORCINE HEART; ELECTRICAL ALTERNANS; MECHANICAL ALTERNANS
SO - Chaos 2000 ;10(2):411-426
104
UI - 15212
AU - Arceo LDB
AU - Cruz-Rivera JJ
AU - Cabanas-Moreno JG
AU - Tsuchiya K
AU - Umemoto M
AU - Calderon H
AD - Zacatenco Inst Politecn Nacl, ESIQIE, Mexico City 07300, DF, Mexico. Zacatenco Inst Politecn Nacl, UPALM, FM, Mexico City 07300, DF, Mexico. Toyohashi Univ Technol, Dept Prod Syst Engn, Toyohashi, Aichi 4418580, Japan
TI - Characterization of Cu-Co alloys produced by mechanosynthesis and spark plasma sintering
AB - Mechanical alloying and sintering by the spark plasma sintering technique have been used to obtain Cu-Co alloys. Microstructure characterization and measurement of magnetic properties are reported. The produced alloys contain 50, 66 and 75 at% Cu. They have been prepared from pure elemental powders in a high-energy planetary mill under an inert Ar atmosphere. Microstructure characterization of the as milled powders has been performed by X-ray diffraction and TEM methods. A supersaturated solid solution is found after 100hr of milling. Sintering produces grains of Cu containing a fine dispersion of Co particles. Similar X-ray diffraction patterns are produced by as milled powders and sintered products. However their magnetic response is different. The magnetic hysteresis curves are measured and important changes in coercive force and magnetization field are found as a function of Co content. Some changes have been observed between the powder and sintered specimens that support the results obtained by the magnetic hysteresis curves
MH - Japan
MH - Mexico|Distrito Federal
T3 - METASTABLEMaterials science forum
PB - ZURICH-UETIKON: TRANS TECH PUBLICATIONS LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Materials Science, Multidisciplinary
U5 - S;Article
NT - SEnglishArticle0BRANDRAIN 6, CH-8707 ZURICH-UETIKON, SWITZERLANDMATER SCI FORUMPart 1&2BQ75R
AV - English
IS - 0255-5476
UR - ISI:000089403900100
SO - 2000 ;():641-646
105
UI - 16625
AU - Archdeacon D
AU - Colbourn CJ
AU - Gitler I
AU - Provan JS
AD - Univ Vermont, Dept Math & Stat, Burlington, VT 05405, USAUniv Vermont, Dept Comp Sci, Burlington, VT 05405, USAInst Politecn Nacl, Ctr Invest & Estudios Avanzados, Dept Matemat, Mexico City 07000, DF, MexicoUniv N Carolina, Chapel Hill, NC 27599, USAArchdeacon, D, Univ Vermont, Dept Math & Stat, Burlington, VT 05405, USA
TI - Four-terminal reducibility and projective-planar wye-delta-wye-reducible graphs
AB - A graph is Y Delta Y-reducible if it can be reduced to a vertex by a sequence of series-parallel reductions and Y Delta Y-transformations. Terminals are distinguished vertices, that cannot be deleted by reductions and transformations. In this article, we show that four-terminal planar graphs are Y Delta Y-reducible when at least three of the vertices lie on the same face. Using this result, we char acterize Y Delta Y-reducible projective-planar graphs. We also consider terminals in projective-planar graphs, and establish that graphs of crossing-number one are Y Delta Y-reducible. (C) 2000 John Wiley & Sons, Inc
MH - Mexico|Distrito Federal
MH - USA
PB - NEW YORK: JOHN WILEY & SONS INC
RP - NOT IN FILE
U3 - TC 3
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0364-9024
UR - ISI:000084904900003
L2 - reducible graphs;terminal;wye-delta;REDUCTION
SO - Journal of Graph Theory 2000 ;33(2):83-93
106
UI - 15382
AU - arcon-Segovia D
AU - Drenkard C
AD - Inst Nacl Nutr Salvador Zubiran, Mexico City 14000, DF, MexicoUniv Cordoba, Cordoba, ArgentinaAlarcon-Segovia, D, Inst Nacl Nutr Salvador Zubiran, Mexico City 14000, DF, Mexico
TI - Vasculitis and the antiphospholipid syndrome
MH - Argentina
MH - Mexico|Distrito Federal
PB - OXFORD: OXFORD UNIV PRESS
RP - NOT IN FILE
U3 - TC 2
U4 - Rheumatology
U5 - J;Letter
AV - English
IS - 1462-0324
UR - ISI:000088892500019
L2 - SYSTEMIC LUPUS-ERYTHEMATOSUS
SO - Rheumatology 2000 ;39(8):922-923
107
UI - 16003
AU - Arcos JA
AU - Garcia HS
AU - Hill CG
AD - Univ Wisconsin, Dept Chem Engn, Madison, WI 53706, USAInst Tecnol Veracruz, Veracruz 91897, MexicoHill, CG, Univ Wisconsin, Dept Chem Engn, 1415 Johnson Dr, Madison, WI 53706 USA
TI - Regioselective analysis of the fatty acid composition of triacylglycerols with conventional high-performance liquid chromatography
AB - A new method for regioselective analysis of triacylglycerols via conventional high-performance liquid chromatography (HPLC) has been developed. The method is simple and avoids the time-consuming purification processes normally characteristic of regioselective analyses. The procedure utilizes an sn-1,3-specific lipase from Rhizopus arrhizus to deacylate the fatty acid residues located at the sn-l and sn-3 positions of triacylglycerols. The fatty acid residues esterified at the sn-2 position are determined by subtraction of the results of the sn-1,3 analysis from an overall composition analysis based on complete saponification of the original sample. The fatty acid mixtures are converted to p-bromophenacyl esters and analyzed using conventional HPLC techniques. The analytical procedure has been verified using a standard structured triacylglycerol. The analytical results for three edible vegetable oils are compared with those obtained via the method proposed by P.J. Williams and co-workers
MH - USA
MH - Mexico|Veracruz
PB - CHAMPAIGN: AMER OIL CHEMISTS SOC A O C S PRESS
RP - NOT IN FILE
U3 - TC 14
U4 - Chemistry, Applied;Food Science & Technology
U5 - J;Article
AV - English
IS - 0003-021X
UR - ISI:000087004800008
L2 - high-performance liquid chromatography;regioselective analysis;Rhizopus arrhizus lipase;triacylglycerols;STEREOSPECIFIC ANALYSIS; TRIGLYCERIDE STRUCTURE; LIPASE; PHASE
SO - Journal of the American Oil Chemists Society 2000 ;77(5):507-512
108
UI - 16052
AU - Arcos JA
AU - Garcia HS
AU - Hill CG
AD - Univ Wisconsin, Dept Chem Engn, Madison, WI 53706, USAInst Tecnol Veracruz, Veracruz 91860, MexicoHill, CG, Univ Wisconsin, Dept Chem Engn, 1415 Engn Dr, Madison, WI 53706 USA
TI - Continuous enzymatic esterification of glycerol with (poly)unsaturated fatty acids in a packed-bed reactor
AB - Enzymatic synthesis of mono-, di-, and triacyglycerols from (poly)unsaturated fatty acids (linoleic, oleic, and conjugated linoleic acids) has been studied as a solvent-free reaction in a packed-bed reactor containing an immobilized lipase from Mucor miehei The extents of the esterification reactions of interest are primarily determined by the molar ratio of glycerol to fatty acid because the presence of excess glycerol as a immiscible phase is responsible for reducing the activity of the water produced by the esterification reactions. For molar ratios of fatty acid to glycerol of less than 1.5, the percentage of the fatty acid esterified decreases quasi-linearly with an increase in this molar ratio. By appropriate manipulation of the fluid-residence time, one can control the relative proportions of the various acylglycerols in the effluent stream. At the outlet of the reactor, one observes excellent spontaneous separation of the glycerol and acylglycerol/fatty acid phases. At 50 degrees C and a fluid residence time of 1 hour, as much as 90% of the fatty acid can be esterified when the molar ratio of fatty acid to glycerol is 0.33 or less. (C) 2000 John Wiley & Sons, Inc
MH - USA
MH - Mexico|Veracruz
PB - NEW YORK: JOHN WILEY & SONS INC
RP - NOT IN FILE
U3 - TC 5
U4 - Biotechnology & Applied Microbiology
U5 - J;Article
AV - English
IS - 0006-3592
UR - ISI:000086928600011
L2 - Mucor miehei lipase;conjugated linoleic acid;(poly)unsaturated fatty acids;synthesis of acylglycerols;(poly)esterification of glycerol;CONJUGATED LINOLEIC-ACID; LIPASES; WATER
SO - Biotechnology and Bioengineering 2000 ;68(5):563-570
109
UI - 14920
AU - Ardila A
AU - Ostrosky-Solis F
AU - Mendoza VU
AD - Inst Colombiano Neuropsicol, Bogota, ColombiaUniv Nacl Autonoma Mexico, Mexico City 04510, DF, MexicoUniv Colima, Colima, MexicoArdila, A, 12230 NW 8 St, Miami, FL 33182, USA
TI - Learning to read is much more than learning to read: A neuropsychologically based reading program
AB - Departing from the observation that illiterates significantly underscore in some neuropsychological tests, a learning-to-read method named NEUROALFA was developed. NEUROALFA is directed to reinforce these underscored abilities during the learning-to-read process. It was administered to a sample of 21 adult illiterates in Colima (Mexico). Results were compared with 2 control groups using more traditional procedures in learning to read. The NEUROPSI neuropsychological test battery was administered to all the participants before and after completing the learning-to-read training program. All 3 groups presented some improvement in the test scores. Gains, however, were significantly higher in the experimental group in Orientation in Time, Digits Backward, Visual Detection, Verbal Memory, Copy of a Semi-Complex Figure, Language Comprehension, Phonological Verbal Fluency, Similarities, Calculation Abilities, Sequences, and all the recall subtests, excluding Recognition. Performance in standard reading tests was also significantly higher in the experimental group. Correlations between pretest NEUROPSI scores and reading ability were low. However; correlations between posttest NEUROPSI scores and reading scores were higher and significant for several subtests. Results are interpreting as supporting the assumption that reinforcement of those abilities in which illiterates significantly underscore results in a significant improvement in neuropsychological test scores and strongly facilitates the learning-to-read process. The NEUROALFA method of teaching reading to adult illiterates is beginning to be used extensively in Mexico. To our knowledge, this is the first attempt to apply neuropsychological principles to social problems
MH - Colombia
MH - Mexico|Colima
MH - Mexico|Distrito Federal
MH - USA
PB - NEW YORK: CAMBRIDGE UNIV PRESS
RP - NOT IN FILE
U3 - TC 10
U4 - Clinical Neurology;Neurosciences;Psychiatry;Psychology
U5 - J;Article
AV - English
IS - 1355-6177
UR - ISI:000165133300006
L2 - illiteracy;reading;neuropsychological testing;cognitive abilities;BRAIN-DAMAGE; TEST-PERFORMANCE; INTELLIGENCE; ILLITERACY; ABILITIES; LITERACY; LANGUAGE
SO - Journal of the International Neuropsychological Society 2000 ;6(7):789-801
110
UI - 15531
AU - Ardila A
AU - Ostrosky-Solis F
AU - Rosselli M
AU - Gomez C
AD - Florida Atlantic Univ, Coll Liberal Arts, Dept Psychol, Div Sci, Davie, FL 33314, USANatl Autonomous Univ Mexico, Mexico City, DF, MexicoRosselli, M, Florida Atlantic Univ, Coll Liberal Arts, Dept Psychol, Div Sci, 3912 Coll Ave, Davie, FL 33314 USA
TI - Age-related cognitive decline during normal aging: The complex effect of education
AB - The purpose of this study was to further analyze the effects of education on cognitive decline during normal aging An 806-subject sample was taken from five different Mexican regions. Participants ranged in age from 16 to 85 years. Subjects were grouped into four educational levels: illiterate, 1-4, 5-9, and 10 or more years of education, and four age ranges: 16-30,31-50, 51-65, and 66-85 years. A brief neuropsychological rest battery (NEUROPSI), standardized and normalized in Spanish, was administered. The NEUROPSI rest battery includes assessment of orientation, attention, memory, language, visuoperceptual abilities, motor skills, and executive functions. In general, test scores were strongly associated with level of educational, and differences among age groups were smaller than differences among education groups. However there was an interaction between age and education such as that among illiterate individuals scores of participants 31-50 years old were higher than scores of participants 16-30 years old for over 50% of the rests. Differ mt patterns of interaction among educational groups were distinguished. It was concluded that: (a) The course of life-span changes in cognition are affected by education. Among individuals with a low level of education, best neuropsychological test performance is observed at an older age than among higher-educated subjects; and (b) there is not a single relationship between age-related cognitive decline and education, but different patterns may be found, depending upon the specific cognitive domain. (C) 2000 National Academy of Neuropsychology. Published by Elsevier Science Ltd
MH - USA
MH - Mexico|Distrito Federal
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 39
U4 - Psychology, Clinical;Psychology
U5 - J;Article
AV - English
IS - 0887-6177
UR - ISI:000088678600003
L2 - aging;neuropsychological testing;cognitive decline;educational effects;MENTAL-STATE-EXAMINATION; NEUROPSYCHOLOGICAL TEST BATTERY; ALZHEIMERS-DISEASE; VISUAL COMPLEXITY; IMAGE AGREEMENT; NAME AGREEMENT; DEMENTIA; LEVEL; POPULATION; PREVALENCE
SO - Archives of Clinical Neuropsychology 2000 ;15(6):495-513
111
UI - 14493
AU - Arenillas I
AU - Arz JA
AD - Univ Zaragoza, Dept Ciencias Tierra Paleontol, E-50009 Zaragoza, SpainUniv Tubingen, Inst & Museum Geol & Palaontol, D-72076 Tubingen, GermanyUniv Autonoma Nuevo Leon, Fac Ciencias Tierra, Linares 67700, MexicoArenillas, I, Univ Zaragoza, Dept Ciencias Tierra Paleontol, E-50009 Zaragoza, Spain
TI - Parvularugoglobigerina eugubina type-sample at Ceselli (Italy): Planktic foraminiferal assemblage and lowermost Danian biostratigraphic implications
AB - The Parvularugoglobigerina eugubina Biozone (lowermost Danian) was defined at Gubbio (Italy) to precisely characterise the Cretaceous/Paleogene (WP) boundary. It was defined by the total range of Pv. eugubina, but this small morphospecies presents some taxonomic problems. The Pv. eugubina holotype and the planktic foraminiferal assemblage of the Pv. eugubina type-sample at Ceselli (Ceselli 3) were revised to precise the biostratigraphic posit ion of this biozone. Of the 21 morphospecies identified in Ceselli 3, 14 are early Paleocene species and 7 are possible Cretaceous "survivors" of the K/P boundary extinction event. To clarify the lowermost Danian biozonation, it was necessary to taxonomically revise Pv. eugubina and Pv. longiapertura, which have both been identified in this sample. Following the definition of Pv, eugubina and the original definition of the nominal biozone, the base of Pv. eugubina Biozone should be placed at the first appearance datum of the eponymous species and not at the first appearance datum of Pv. longiapertura
MH - Germany
MH - Mexico|Nuevo Leon
MH - Spain
PB - MILANO: UNIV STUDI MILANO
RP - NOT IN FILE
U3 - TC 5
U4 - Geology;Paleontology
U5 - J;Article
AV - English
IS - 0035-6883
UR - ISI:000166376300008
L2 - planktic foraminifera;taxonomy;biostratigraphy;K/P boundary;Paleocene;Gubbio;CRETACEOUS-TERTIARY BOUNDARY; GLOBAL IMPLICATIONS; ANTARCTIC OCEAN; MASS EXTINCTION; TRANSITION; TRISERIAL; RADIATION; TURNOVER; BISERIAL; TUNISIA
SO - Rivista Italiana di Paleontologia e Stratigrafia 2000 ;106(3):379-390
112
UI - 15468
AU - Arenillas I
AU - Arz JA
AU - Molina E
AU - Dupuis C
AD - Univ Zaragoza, Dept Ciencias Tierra, Area Paleontol, E-50009 Zaragoza, SpainUniv Autonoma Nuevo Leon, Fac Ciencias Tierra, Linares 67700, MexicoFac Polytech Mons, Lab Geol Fondamentale & Appl, B-7000 Mons, BelgiumArenillas, I, Univ Zaragoza, Dept Ciencias Tierra, Area Paleontol, E-50009 Zaragoza, Spain
TI - The Cretaceous/Paleogene (K/P) boundary at Ain Settara, Tunisia: Sudden catastrophic mass extinction in planktic foraminifera
AB - The quantitative study and high resolution sampling of an essentially continuous and expanded Cretaceous/Paleogene (K/P) boundary section in Tunisia allow us to test the model of extinction in planktic foraminifera. The extinction at the Ain Settara section occurred over a short period of time similar to the Tunisian sections at El Kef and Elles and the Spanish sections at Agost, Caravaca and Zumaya, At Ain Settara only 3 species disappeared in the latest Maastrichtian, 45 became extinct precisely at the Km boundary and 18 disappeared in the earliest Danian. The species that became extinct at the K/P boundary constitute about 20% of the individuals in the population larger than 63 microns and 68% of the species, which suddenly became extinct in a catastrophic event precisely coinciding with the layer containing evidence for an asteroid impact. Most of these species are large, complex and low latitude deeper to intermediate dwelling forms. This extinction event is clearly the most important catastrophic mass extinction recorded in the history of planktic foraminifera. This pattern of extinction is superimposed on a controversial gradual pattern of extinction of 21 species that apparently began in the latest Maastrichtian and ended in the early Danian, The Maastrichtian species that seem to become extinct gradually are generally small, cosmopolitan and simple surface dwellers. The catastrophic mass extinction of the 45 species coincident with the K/P boundary is compatible with the effect of the impact of a large asteroid, whereas the gradual extinction of 18 species in the basal Danian could also be attributed to the long term disruptive effect of the impact
MH - Belgium
MH - Mexico|Nuevo Leon
MH - Spain
PB - CAMBRIDGE: CUSHMAN FOUNDATION FORAMINIFERAL RES
RP - NOT IN FILE
U3 - TC 16
U4 - Paleontology
U5 - J;Article
AV - English
IS - 0096-1191
UR - ISI:000088811700004
L2 - KEF BLIND TEST; TERTIARY BOUNDARY; EL-KEF; CRETACEOUS/TERTIARY BOUNDARY; ENVIRONMENTAL-CHANGES; SE SPAIN; TEST II; SURVIVORSHIP; CARAVACA; SECTIONS
SO - Journal of Foraminiferal Research 2000 ;30(3):202-218
113
UI - 15954
AU - Arenillas I
AU - Arz JA
AU - Molina E
AU - Dupuis C
AD - Univ Zaragoza, Dept Ciencias Tierra Paleontol, E-50009 Zaragoza, SpainUniv Tubingen, Inst Museum Geol & Palaontol, D-72076 Tubingen, GermanyUniv Autonoma Neuvo Leon, Fac Ciencias Tierra, Linares 67700, MexicoFac Polytech Mons, Lab Geol Fondamentale & Appliquee, B-7000 Mons, BelgiumArenillas, I, Univ Zaragoza, Dept Ciencias Tierra Paleontol, E-50009 Zaragoza, Spain
TI - An independent test of planktic foraminiferal turnover across the Cretaceous/Paleogene (K/P) boundary at El Kef, Tunisia: Catastrophic mass extinction and possible survivorship
AB - Planktic foraminiferal biostratigraphy and assemblage turnover across the Cretaceous/Paleogene (WP) boundary at EI Kef revealed the largest and most abrupt extinction event in the history of planktic foraminifera. Cretaceous assemblages were very abundant and diverse and included 67 stable identified species within the terminal Maastrichtian. The mass extinction was characterized by the disappearance of 6 (8.9%) species in the last 12 meters of the upper Maastrichtian and the extinction of 46 (68.7%) species at the WP boundary as well as 15 (22.4%) possible survivors ranging into the lowermost Danian. The range of planktic foraminifera only based on six samples (equivalent to the previous El Kef blind sample test) showed an even more catastrophic extinction pattern, with only I species disappearing before the WP boundary. The WP debate is the result of several problems which include the "Signor-Lipps" effect, the possibility of reworking and the existence of hiatuses. However, irrespective of the different interpretations we conclude that there were no significant extinction nor quantitative changes before the WP boundary and that most Cretaceous species suddenly became extinct at the WP boundary. The El Kef section is one of the most continuous marine WP boundary sections known and hiatuses have not been identified. Furthermore, possible Cretaceous survivors had a smaller size and lower absolute abundance in the lower Danian than in the upper Maastrichtian and the planktic foraminiferal evolutionary radiation began above the WP boundary and not below. The same results have been found in other subtropical-temperate sections and may be sufficient proof for the existence of a catastrophic mass extinction at the WP boundary. The planktic foraminiferal WP extinction pattern is also very compatible with the catastrophic effects caused by the impact of a large extra-terrestrial asteroid
MH - Belgium
MH - Germany
MH - Mexico|Nuevo Leon
MH - Spain
PB - NEW YORK: MICROPALEONTOLOGY PRESS
RP - NOT IN FILE
U3 - TC 17
U4 - Paleontology
U5 - J;Article
AV - English
IS - 0026-2803
UR - ISI:000087269400002
L2 - BLIND TEST I; TERTIARY BOUNDARY; CRETACEOUS/TERTIARY BOUNDARY; GLOBAL IMPLICATIONS; ANTARCTIC OCEAN; BASQUE COUNTRY; HIGH-LATITUDES; CARAVACA; SPAIN; BIOSTRATIGRAPHY
SO - Micropaleontology 2000 ;46(1):31-49
114
UI - 16374
AU - Arenillas I
AU - Arz JA
AU - Molina E
AD - Univ Zaragoza, Dept Ciencias Tierra, ES-50009 Zaragoza, SpainUniv Autonoma Nuevo Leon, Fac Ciencias Tierra, MEX-67700 Linares, NL, MexicoArenillas, I, Univ Zaragoza, Dept Ciencias Tierra, ES-50009 Zaragoza, Spain
TI - Spanish and Tunisian Cretaceous/Tertiary boundary sections: A planktic foraminiferal biostratigraphic comparison and evolutionary events
MH - Mexico|Nuevo Leon
MH - Spain
PB - UPPSALA: SWEDISH SCIENCE PRESS
RP - NOT IN FILE
U3 - TC 1
U4 - Geology;Paleontology
U5 - J;Article
AV - English
IS - 1103-5897
UR - ISI:000085853400004
L2 - EXTINCTION
SO - Gff 2000 ;122():11-12
115
UI - 15651
AU - Arizaga S
AU - Ezcurra E
AU - Peters E
AU - de Arellano FR
AU - Vega E
AD - Univ Nacl Autonoma Mexico, Inst Ecol, Morelia 58190, Michoacan, MexicoSan Diego Nat Hist Museum, Biodivers Res Ctr Californias, San Diego, CA 92112, USAArizaga, S, Univ Nacl Autonoma Mexico, Inst Ecol, Apartado Postal 27-3 Xangari, Morelia 58190, Michoacan, Mexico
TI - Pollination ecology of Agave macroacantha (Agavaceae) in a Mexican tropical desert. I. Floral biology and pollination mechanisms
AB - In a study of sexual reproduction in long-lived semelparous plants, we observed Agave macroacantha in the tropical desert of Tehuacan-Cuicatlan, Mexico, describing duration of flowering, flower phenology, and nectar production patterns. We also performed two manipulative experiments evaluating (a) the seed production efficiency of different crossing systems (selfing, cross-pollination. apomixis. and control), and (b) the effect of different pollinators (diurnal exposure to pollinators, nocturnal exposure, exclusion, and control) on the seeds produced. Flowering occurred from early May to late July and had a mean duration of 29 days in the individual rosettes. The flowers were protandrous; anthesis occurred in the afternoon of the third day after floral opening, and the pistils matured in the afternoon of the fifth day. The stigmas remained receptive from dusk to the following morning. Pollination was mostly allogamous. Nectar was produced principally during the night, from the first stages of floral aperture until the stigmas wilted and flowering ceased. The flowers were visited during the day by hymenoptera, butterflies, and hummingbirds and during the night by bats and moths. Only the nocturnal visitors, however, were successful pollinators. Agave macroacanthus is extremely dependent on nocturnal pollinators for its reproductive success
MH - Mexico|Michoacan
MH - USA
PB - COLUMBUS: BOTANICAL SOC AMER INC
RP - NOT IN FILE
U3 - TC 15
U4 - Plant Sciences
U5 - J;Article
AV - English
IS - 0002-9122
UR - ISI:000088235300013
L2 - Agave macroacantha;Agavaceae;nectar;nectar-feeding bats;pollination biology;rosette plants;tropical deserts;BATS; NECTAR
SO - American Journal of Botany 2000 ;87(7):1004-1010
116
UI - 15652
AU - Arizaga S
AU - Ezcurra E
AU - Peters E
AU - de Arellano FR
AU - Vega E
AD - Univ Nacl Autonoma Mexico, Inst Ecol, Morelia 58190, Michoacan, MexicoSan Diego Nat Hist Museum, Biodivers Res Ctr Californias, San Diego, CA 92112, USAArizaga, S, Univ Nacl Autonoma Mexico, Inst Ecol, Apartado Postal 27-3 Xangari, Morelia 58190, Michoacan, Mexico
TI - Pollination ecology of Agave macroacantha (Agavaceae) in a Mexican tropical desert. II. The role of pollinators
AB - We did a series of observational studies and manipulative experiments on the guild of nocturnal visitors of Agave macroacantha, including (1) a description of the hourly patterns of visits by moths and bats, (2) an evaluation of the relative contribution of bats and moths to flowering success, and (3) an evaluation of the pollination efficiency of the different bar species. Scapes exposed to moths but excluded to bats yielded similar to 50% fewer fruits than those exposed to both pollinator groups. Flowers exposed to the bat species Leptonycteris curasoae showed similar fruiting success to those exposed to Choeronycteris mexicana and to those exposed to the whole nocturnal visitor guild. However, the fruits originated from flowers pollinated by Lepronycteris curasoae yielded significantly more seed than those exposed to Choeronycteris mexicana or to the whole pollinator guild. It is concluded that Agave macroocantha is extremely dependent on nocturnal pollinators for its reproductive success and that bats are especially important for successful pollination. Some of these pollinators are migratory and have been reported to be steadily declining. A continuing decline in the populations of pollinators may impede the successful sexual reproduction of the plant host and may put the long-term survival of this agave species under risk
MH - Mexico|Michoacan
MH - USA
PB - COLUMBUS: BOTANICAL SOC AMER INC
RP - NOT IN FILE
U3 - TC 11
U4 - Plant Sciences
U5 - J;Article
AV - English
IS - 0002-9122
UR - ISI:000088235300014
L2 - Agave macroacantha;deserts;fruit set;Mexico;moths;nectar-feeding bats;pollination biology;pollinator effectiveness;rosette plants;NECTAR-FEEDING BATS
SO - American Journal of Botany 2000 ;87(7):1011-1017
117
UI - 15748
AU - Arkin RC
AU - Ali K
AU - Weitzenfeld A
AU - Cervantes-Perez F
AD - Georgia Tech, Coll Comp, Atlanta, GA 30332, USAInst Technol Autonomo Mexico, Dept Acad Computac, Mexico City, DF, MexicoArkin, RC, Georgia Tech, Coll Comp, Atlanta, GA 30332, USA
TI - Behavioral models of the praying mantis as a basis for robotic behavior
AB - Formal models of animal sensorimotor behavior can provide effective methods for generating robotic intelligence. In this article we describe how schema-theoretic models of the praying mantis derived from behavioral and neuroscientific data can be implemented on a hexapod robot equipped with a real time color vision system. This implementation incorporates a wide range of behaviors, including obstacle avoidance, prey acquisition, predator avoidance, mating, and chantlitaxia behaviors that can provide guidance to neuroscientists, ethologists, and roboticists alike. The goals of this study are threefold: to provide an understanding and means by which fielded robotic systems are not competing with other agents that are more effective at their designated task; to permit them to be successful competitors within the ecological system and capable of displacing less efficient agents; and that they are ecologically sensitive so that agent-environment dynamics are well-modeled and as predictable as possible whenever new robotic technology is introduced. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Distrito Federal
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 8
U4 - Automation & Control Systems;Computer Science, Artificial Intelligence;Robotics
U5 - J;Article
AV - English
IS - 0921-8890
UR - ISI:000087800700003
L2 - schema-based control;behavior-based robotics;praying mantis behavior;MOBILE ROBOT; NAVIGATION; MECHANISMS; SCHEMA; SYSTEM
SO - Robotics and Autonomous Systems 2000 ;32(1):39-60
118
UI - 15660
AU - Armaroli T
AU - Trombetta M
AU - Alejandre AG
AU - Solis JR
AU - Busca G
AD - Univ Genoa, Dipartimento Ingn Chim & Proc, I-16129 Genoa, ItalyUNAM, Fac Quim, Dept Ingn Quim, UNICAT, Mexico City 04510, DF, MexicoArmaroli, T, Univ Genoa, Dipartimento Ingn Chim & Proc, P JF Kennedy, I-16129 Genoa, Italy
TI - FTIR study of the interaction of some branched aliphatic molecules with the external and internal sites of H-ZSM5 zeolite
AB - The interaction of the branched molecules pivalonitrile (2,2-dimethylpropionitrile, PN), methyl tert-butyl ether (MTBE), tert-butyl alcohol (TBA), and 2,2-dimethylbutane (DMB), as well as of methylcyclohexane, benzonitrile and benzene over different H-ZSM5 zeolite samples was investigated by FTIR spectroscopy. PN does not enter the cavities of MFI structures at room temperature and 0-25 Torr pressure, at least when Al content is quite high. Also, TBA and MTBE do not enter the cavities under these conditions although isobutene produced by their decomposition, easily enters and polymerizes in the internal acidic sites. Conversely, DMB slowly enters the MFI zeolite cavities. On the other hand, the co-presence of benzene allows PN to enter the cavities and to interact with the internal sites. This shows that the access of single molecules can be influenced by other molecules in a mixture. The experiments also confirmed that two kinds of terminal silanol groups, indistinguishable from the point of view of the OH stretching band but differing in their Bronsted acidity, are located at the external surface of the ZSM5 zeolite crystals. Additionally, it was established that the external ZSM5 zeolite surface, even for low Al content samples, contains two types of Lewis acid sites. Conversely, no evidence was found for the presence of bridging Si-(OH)-Al sites at the external surface of the ZSM5 zeolite samples. This further corroborates the proposal that the bridging "zeolitic'' Bronsted acid sites are actually formed as a consequence of the porous structure of the zeolites and do not simply arise from the substitution of Al for silicon in a silica framework
MH - Italy
MH - Mexico|Distrito Federal
PB - CAMBRIDGE: ROYAL SOC CHEMISTRY
RP - NOT IN FILE
U3 - TC 30
U4 - Chemistry, Physical;Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 1463-9076
UR - ISI:000088087100032
L2 - SKELETAL ISOMERIZATION CATALYSIS; SURFACE-ACIDITY; IR; FERRIERITE; SILICALITE; ZSM-5; AL; CO
SO - Physical Chemistry Chemical Physics 2000 ;2(14):3341-3348
119
UI - 16647
AU - Armas B
AU - Herrera MD
AU - Sibieude F
AD - CNRS, Inst Sci & Genie Mat & Procedes, F-66125 Font Romeu, FranceHerrera, MD, UNAM, Dept Fis Aplicada & Tecnol Avanzada, Inst Fis, Apdo Postal 1-1010, Queretaro 76000, Mexico
TI - Deposition of aluminium nitride coatings using a cold wall CVD reactor
AB - Aluminium nitride was obtained in a cold wall reactor using AlCl3 and NH3 as precursors and N-2 as a carrier gas. AlCl3 was synthesized in situ by means of an original method based on the SiCl4,(g) reaction on Al(s). The substrate used is a cylinder of graphite coated with SiC and heated by high frequency induction. The deposition rate was studied as a function of temperature in the range 900-1500 degrees C, the total pressure varying from 2 to 180 hPa. At low temperatures an Arrhenius type representation of the kinetics for several pressures indicated a thermally activated behaviour with an apparent activation energy of about 80 kJ mol(-1). At high deposition temperatures the deposition rate was almost constant, indicating that the growth is controlled by the diffusion process. The influence of gas composition and total AlCl3 flow rate was also discussed. The different layers were characterized particularly by means of X-ray diffraction and scanning electron microscopy. The influence of temperature and total pressure on crystallization and morphology was studied. (C) 2000 Elsevier Science S.A. All rights reserved
MH - France
MH - Mexico|Queretaro
PB - LAUSANNE: ELSEVIER SCIENCE SA
RP - NOT IN FILE
U3 - TC 1
U4 - Materials Science, Coatings & Films;Physics, Applied
U5 - J;Article
AV - English
IS - 0257-8972
UR - ISI:000084717100016
L2 - aluminium nitride;chemical vapour deposition;CHEMICAL-VAPOR-DEPOSITION; ALN FILMS; GROWTH; AIN
SO - Surface & Coatings Technology 2000 ;123(2-3):199-203
120
UI - 15349
AU - Armitage P
AU - Healy MJR
AU - Cox DR
AU - Nelder J
AU - Dawid AP
AU - Kingman JFC
AU - Bartholomew DJ
AU - O'Hagan A
AU - Hand DJ
AU - Barnard G
AU - Efron B
AU - Sprott DA
AU - Evett IW
AU - Lindley D
AD - Univ London Imperial Coll Sci Technol & Med, London, EnglandUniv Coll London, London WC1E 6BT, EnglandUniv Bristol, Bristol BS8 1TH, Avon, EnglandUniv Sheffield, Sheffield S10 2TN, S Yorkshire, EnglandStanford Univ, Stanford, CA 94305, USACtr Invest Matemat, Guanajuato, MexicoForens Sci Serv, London, England
TI - The philosophy of statistics - Comments
MH - United Kingdom
MH - Mexico|Guanajuato
MH - USA
PB - OXFORD: BLACKWELL PUBL LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Statistics & Probability
U5 - J;Editorial Material
AV - English
IS - 0039-0526
UR - ISI:000088997300002
L2 - FORENSIC IDENTIFICATION; INFERENCE; BOOTSTRAP; SCIENCE; BAYES
SO - Journal of the Royal Statistical Society Series D-the Statistician 2000 ;49():319-337
121
UI - 14918
AU - Arnaudeau C
AU - Miranda ET
AU - Jenssen D
AU - Helleday T
AD - Univ Stockholm, Wallenberg Lab, Dept Genet & Cellular Toxicol, S-10691 Stockholm, SwedenAutonomous Univ Madrid, UNAM, Fac Chem, Dept Inorgan & Nucl Chem, Mexico City, DF, MexicoArnaudeau, C, Univ Stockholm, Wallenberg Lab, Dept Genet & Cellular Toxicol, S-10691 Stockholm, Sweden
TI - Inhibition of DNA synthesis is a potent mechanism by which cytostatic drugs induce homologous recombination in mammalian cells
AB - Recombination is a process thought to be underlying genomic instability involved in carcinogenesis. This report examines the potential of cytostatic drugs to induce intrachromosomal homologous recombination, Tn order to address this question, the hprt gene of a well-characterized mammalian cell line was employed as a unique endogenous marker for homologous recombination. Commonly used cytostatic drugs with different mode of action were investigated in this context, i.e. bifunctional alkylating agents, inhibitors of DNA synthesis, inhibitors of topoisomerases and a spindle poison. With the exception of the spindle poison, all these drugs were found to induce homologous recombination, with clear differences in their recombination potency, which could be related to their mechanism of action. Bifunctional alkylating agents were the least efficient, whereas inhibitors of DNA synthesis were found to be the most potent inducers of homologous recombination. This raises the question whether these later drugs should be considered for adverse effects in cancer chemotheraphy. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Distrito Federal
MH - Sweden
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 24
U4 - Biotechnology & Applied Microbiology;Genetics & Heredity;Toxicology
U5 - J;Article
AV - English
IS - 0921-8777
UR - ISI:000165203800006
L2 - cytostatic drugs;recombination;V79 Chinese hamster cell;hypoxanthine guanine phosphoribosyltransferase;CHINESE-HAMSTER CELLS; SISTER-CHROMATID EXCHANGES; MITOTIC RECOMBINATION; ANTICANCER DRUGS; INTRACHROMOSOMAL RECOMBINATION; CHROMOSOMAL-ABERRATIONS; GENE AMPLIFICATION; HUMAN CANCER; IN-VITRO; AGENTS
SO - Mutation Research-Dna Repair 2000 ;461(3):221-228
122
UI - 16316
AU - Arora P
AU - Kausz AT
AU - Obrador GT
AU - Ruthazer R
AU - Khan S
AU - Jenuleson CS
AU - Meyer KB
AU - Pereira BJG
AD - Tufts Univ, Sch Med & Dialysis Clin Inc, New England Med Ctr, Tupper Res Inst,Div Nephrol, Boston, MA 02111, USATufts Univ, Sch Med & Dialysis Clin Inc, New England Med Ctr, Tupper Res Inst,Div Clin Care Res, Boston, MA 02111, USAPanamer Univ, Sch Med, Mexico City, DF, MexicoPereira, BJG, Tufts Univ, Sch Med & Dialysis Clin Inc, New England Med Ctr, Tupper Res Inst,Div Nephrol, 750 Washington St, Boston, MA 02111 USA
TI - Hospital utilization among chronic dialysis patients
AB - Factors driving inpatient and outpatient utilization were studied among patients who began dialysis for chronic renal failure at the New England Medical Center (NEMC) between 1992 and 1997. Clinical, laboratory, and hospital resource utilization data were obtained from patient records and electronic databases. There were 2.2 hospitalizations and 14.8 hospital days per patient year at risk (PYAR). The number of hospitalizations and hospital days per PYAR were higher in the first 3 mo of initiating dialysis (4.3 and 28.3, respectively) compared to after 3 mo (1.9 and 12.9, respectively). Factors associated with increased risk of hospital days within the first 3 mo included non-health maintenance organization insurance, ischemic heart disease, late referral to the nephrologist, and use of temporary vascular access for the first dialysis. Patients with ischemic heart disease and who received dialysis during the years 1992-1994 compared with 1996-1997 had an increased risk of hospital days after 3 mo of initiating dialysis. There were 16.6 outpatient visits per PYAR, with significant differences in utilization between the first 3 mo and after 3 mo of initiating dialysis. Thus, hospital utilization was significantly higher in the first 3 mo compared to after 3 mo, and factors associated with hospital utilization depended on duration of dialysis. In particular, delayed referral to the nephrologist and lack of permanent vascular access were independently associated with increased risk of hospital utilization in the first 3 mo of dialysis. Greater attention to timely referral to the nephrologist and timely placement of vascular access could result in reduced utilization and cost savings
MH - Mexico|Distrito Federal
MH - USA
PB - PHILADELPHIA: LIPPINCOTT WILLIAMS & WILKINS
RP - NOT IN FILE
U3 - TC 39
U4 - Urology & Nephrology
U5 - J;Article
AV - English
IS - 1046-6673
UR - ISI:000086046900017
L2 - HEMODIALYSIS-PATIENTS; VASCULAR ACCESS; MANAGED-CARE; PHYSICIANS; MORBIDITY; MEDICARE; FAILURE; COSTS; RISK
SO - Journal of the American Society of Nephrology 2000 ;11(4):740-746
123
UI - 15385
AU - Arreaga G
AU - Cho IY
AU - Guven J
AD - Inst Politecn Nacl, Ctr Invest & Estudios Avanzados, Dept Fis, Mexico City 07000, DF, MexicoEmory Univ, Dept Phys, Atlanta, GA 30322, USANatl Autonomous Univ Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoArreaga, G, Inst Politecn Nacl, Ctr Invest & Estudios Avanzados, Dept Fis, Apdo Postal 14-740, Mexico City 07000, DF, Mexico
TI - Stability of self-gravitating magnetic monopoles
AB - The stability of a spherically symmetric self-gravitating magnetic monopole is examined in the thin wall approximation: modeling the interior false vacuum as a region of de Sitter space; the exterior as an asymptotically Rat region of the Reissner-Nordstrom geometry; and the boundary separating the two as a charged domain wall. There remains only to determine how the wall gets embedded in these two geometries. In this approximation, the ratio k of the false Vacuum to surface energy densities is a measure of the symmetry breaking scale eta. Solutions are characterized by this ratio, the charge on the wall Q, and the value of the conserved total energy M. We find that for each fixed k and Q up to some critical value, there exists a unique globally static solution, with M similar or equal to Q(3/2); any stable radial excitation has M hounded above by Q, the value assumed in an extremal Reissner-Nordstrom geometry, and these are the only solutions with M < Q. As M is raised above Q a black hole forms in the exterior: (i) for low Q or k, the wall is crushed; (ii) for higher values, it oscillates inside the black hole. If the mass is not too high the former solutions coexist with an inflating bounce: (iii) for k, Q or M outside the above regimes, there is a unique inflating solution. In case (i) the course of the bounce lies within a single asymptotically Rat region (AFR) and it resembles closely the bounce exhibited by a false vacuum bubble (with Q = 0). In case (iii) the course of the bounce spans two consecutive AFRs. However, for an asymptotic observer it resembles a monotonic false vacuum bubble
MH - Mexico|Distrito Federal
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 2
U4 - Astronomy & Astrophysics;Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 0556-2821
UR - ISI:000088793100035
L2 - GLOBAL MONOPOLES; VACUUM BUBBLES; BLACK-HOLES; DYNAMICS; UNIVERSE; INFLATION; FIELD; MODEL
SO - Physical Review D 2000 ;62(4):art-043520
124
UI - 16597
AU - Arreaga G
AU - Lopez-Bonilla JL
AU - Ovando G
AD - IPN, Ctr Invest & Estudios Avanzados, Mexico City 0700, DF, MexicoInt Inst Integral Human Sci, Montreal, PQ H3H 1K5, CanadaUniv Autonoma Metropolitana Azcapotzalco, Div CBI, Area Fis, Mexico City 02200, DF, Mexico
TI - Lanczos spintensor and Lienard Wiechert field
AB - This paper proves that the analogies between the Lanczos spintensor K-abc for the conformal tensor of the spacetime and the Weert potential K-B(ijc) for the bounded part of the Lienard-Wiechert field allows to construct generators for the last one, which is important for the electrodynamics of classical charged particles
MH - Canada
MH - Mexico|Distrito Federal
PB - NEW DELHI: INDIAN NAT SCI ACAD
RP - NOT IN FILE
U3 - TC 2
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0019-5588
UR - ISI:000084949700008
L2 - Lanczos superpotential;splitting and generators for the Weert potential;potentials for the Lienard-Wiechert field;MAXWELL TENSOR; WAVE-EQUATION
SO - Indian Journal of Pure & Applied Mathematics 2000 ;31(1):85-91
125
UI - 14721
AU - Arrizon V
AU - Testorf M
AU - Sinzinger S
AU - Jahns J
AD - Inst Nacl Astrofis Opt & Elect, Puebla 72000, PU, MexicoUniv Massachusetts, Dept Elect & Comp Engn, Lowell, MA 01854, USAFern Univ Hagen, LG Opt Nachrichtentech, D-58084 Hagen, GermanyArrizon, V, Inst Nacl Astrofis Opt & Elect, Apartado Postal 216, Puebla 72000, PU, Mexico
TI - Iterative optimization of phase-only diffractive optical elements based on a lenslet array
AB - We describe the design of Fourier-type phase-only array generators. The numerical optimization employs the Fienup algorithm, where the parageometric design of the phase retardation profile, with the form of a lenslet array, is used as the initial guess of the optimization process. This approach provides designs with high performance that can be obtained with comparatively low computing effort. This is particularly true for elements generating large spot arrays. For symmetric reconstruction fields, the optimized phase profile typically has the same symmetry as that for the reconstruction field and can be easily unwrapped. (C) 2000 Optical Society of America [S0740-3232(00)02612-0] OCIS codes: 050.1970, 200.4650, 070.2580, 090.1760
MH - Germany
MH - Mexico|Puebla
MH - USA
PB - WASHINGTON: OPTICAL SOC AMER
RP - NOT IN FILE
U3 - TC 6
U4 - Optics
U5 - J;Article
AV - English
IS - 0740-3232
UR - ISI:000165752300004
L2 - DESIGN; EFFICIENCY; GRATINGS
SO - Journal of the Optical Society of America A-Optics Image Science and Vision 2000 ;17(12):2157-2164
126
UI - 15927
AU - Arrizon V
AU - Rojo-Velazquez G
AU - Ibarra JG
AD - Inst Nacl Astrofis Opt & Elect, Puebla 72000, MexicoUniv Arkansas, Fayetteville, AR 72701, USAArrizon, V, Inst Nacl Astrofis Opt & Elect, Apdo Postal 216, Puebla 72000, Mexico
TI - Fractional Talbot effect: Compact description
AB - We present a compact description of the fractional Talbot effect, with the simplest expression for the Fresnel field of a grating, together with the simplest polar formulas for Talbot coefficients
MH - Mexico|Puebla
MH - USA
PB - TOKYO: OPTICAL SOC JAPAN
RP - NOT IN FILE
U3 - TC 3
U4 - Optics
U5 - J;Review
AV - English
IS - 1340-6000
UR - ISI:000087403900006
L2 - diffraction;Talbot effect;fractional Talbot effect;MULTILEVEL PHASE GRATINGS; ARRAY ILLUMINATORS; EQUATIONS
SO - Optical Review 2000 ;7(2):129-131
127
UI - 15982
AU - Arroyo M
AU - Zitzumbo R
AU - Avalos F
AD - CSIC, Inst Ciencia & Tecnol Polimeros, E-28006 Madrid, SpainCiatec A C, Guanajuato, MexicoUniv Aut Coahuila, Saltillo 25000, Coahuila, MexicoArroyo, M, CSIC, Inst Ciencia & Tecnol Polimeros, Juan Cierva 3, E-28006 Madrid, Spain
TI - Composites based on PP/EPDM blends and aramid short fibres. Morphology/behaviour relationship
AB - The effect of both a thermoplastic elastomer (EPDM) and short aramid fibres on polypropylene (PP) crystallization kinetics and tensile behaviour has been investigated. The results have shown that PP/EPDM blends are non-miscible in the melt, and, at low EPDM percentages in the blend (<25%), the particles of EPDM act as nucleating agents and co-crystallize with PP. However, at higher percentages, the EPDM obstructs the mobility of PP chains and hence decreases the PP crystallization rate. Aramid fibres are effective nucleating agents for PP crystallization, giving rise to the phenomenon of PP transcrystallinity on their surface. The tensile behaviour of the blends and composites are in intimate relation with the morphological characteristics of these materials. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Mexico|Coahuila
MH - Mexico|Guanajuato
MH - Spain
PB - OXFORD: ELSEVIER SCI LTD
RP - NOT IN FILE
U3 - TC 31
U4 - Polymer Science
U5 - J;Article
AV - English
IS - 0032-3861
UR - ISI:000087123900036
L2 - composites;PP/EPDM blends;aramid short fibres;MECHANICAL-PROPERTIES RELATIONSHIPS; ISOTACTIC POLYPROPYLENE; TRANSCRYSTALLINITY PHENOMENA; CRYSTALLIZATION
SO - Polymer 2000 ;41(16):6351-6359
128
UI - 16081
AU - Arroyo M
AU - Bernes S
AU - Brianso JL
AU - Mayoral E
AU - Richards RL
AU - Rius J
AU - Torrens H
AD - Natl Autonomous Univ Mexico, Fac Quim, DEPg, Mexico City 04510, DF, MexicoBUAP, Inst Ciencias, Ctr Quim, Puebla 72570, MexicoUniv Autonoma Barcelona, Fac Ciencias, Unidad Cristalog, E-08193 Barcelona, SpainJohn Innes Ctr Plant Sci Res, Norwich NR4 7UH, Norfolk, EnglandCSIC, Inst Ciencia Mat Barcelona, E-08193 Barcelona, SpainTorrens, H, Natl Autonomous Univ Mexico, Fac Quim, DEPg, Cd Univ, Mexico City 04510, DF, Mexico
TI - C-F bond activation in polyfluorobenzothiolate compounds of Os(III). X-ray structures of [Os(SC6F4(F-2))(SC6F5)(2)(PMe2Ph)(2)], [Os(SC6F5)(2)(o-S2C6F4)(PMe2Ph)] and [Os(C6F5)(2)(o-S2C6F4)(PMe2Ph)(2)]
AB - Thermolysis of [Os(SR)(3)(PMe2Ph)(2)] (R = C6F5 (1a) or C6HF4-4 (1b)) in refluxing toluene affords [Os(SC6F5)(2)(o-S2C6F4)(PMe2Ph)] (2a), [Os(SC6HF4)(2)(o-S2C6HF3)(PMe2Ph)] (2b), and [Os(C6F5)(2)(o-S2C6F4)(PMe2Ph)(2)] (3a) through processes involving C-F and C-S bond cleavage as well as rearrangement of C-S bonds. The single-crystal diffraction structures of la, 2a and 3a have been determined. In the solid state compound 1a shows a C-F --> Os interaction. (C) 2000 Elsevier Science S.A. All rights reserved
MH - United Kingdom
MH - Mexico|Distrito Federal
MH - Mexico|Puebla
MH - Spain
PB - LAUSANNE: ELSEVIER SCIENCE SA
RP - NOT IN FILE
U3 - TC 12
U4 - Chemistry, Inorganic & Nuclear;Chemistry, Organic
U5 - J;Article
AV - English
IS - 0022-328X
UR - ISI:000086737800010
L2 - C-F bond activation;polyfluorobenzothiolate;osmium;thermolysis;CARBON-FLUORINE BONDS; CRYSTAL-STRUCTURES; METAL-COMPLEXES; RHODIUM; RU(SC6F4(F-2))(SC6F5)2(PME2PH)2; REGIOSELECTIVITY; DERIVATIVES; MECHANISM; CLEAVAGE; LIGANDS
SO - Journal of Organometallic Chemistry 2000 ;599(2):170-177
129
UI - 15929
AU - Arroyo P
AU - Loria A
AU - Fernandez V
AU - Flegal KM
AU - Kuri-Morales P
AU - Olaiz G
AU - Tapia-Conyer R
AD - Mexican Hlth Fdn, Hyattsville, MD, USANatl Inst Nutr Salvador Zubiran, Hyattsville, MD, USACtr Dis Control & Prevent, Natl Ctr Hlth Stat, Hyattsville, MD 20782, USAArroyo, P, Perifer Sur 4809 Arenal Tepepan, Mexico City 14610, DF, Mexico
TI - Prevalence of pre-obesity and obesity in urban adult Mexicans in comparison with other large surveys
AB - Objective: 1. To estimate the prevalence of pre-obesity and obesity in a 1992 to 1993 national survey of the Mexican urban adult population. 2. To compare our findings with other national surveys and with data for Mexican Americans. Research Methods and Procedures: The national representative sample of the Mexican urban adult population included 8462 women and 5929 men aged 20 to 69 years from 417 towns of >2500 people. Body mass index (BMI), calculated from measured weight and height, was classified using the World Health Organization categories of underweight (BMI < 18.5 kg/m(2)), normal weight (BMI 18.5 to 24.9 kg/m(2)), pre-obesity (PreOB = BMI 25 to 29.9 kg/m(2)) and obesity (OB = BMI 30+ kg/m(2)). Estimates for Mexican Americans were calculated from U.S. survey data. Results: Overall, 38% of the Mexican urban adult population were classified as pre-obese and 21% as obese. Men had a higher prevalence of pre-obesity than women did at all ages, but women had higher values of obesity. Both pre-obesity and obesity increased with age up to the age range brackets of 40 to 49 or 50 to 59 years for both men and women. Both pre-obesity and obesity prevalence estimates were remarkably similar to data for Mexican Americans from 1982 through 1984. Comparison with other large surveys showed that countries differed more in the prevalence of obesity than of pre-obesity, leading to differences in the PreOB/OB ratio, and that countries also differed in the gender ratio (female/male) for both pre-obesity and obesity. Discussion: Pre-obesity and obesity were high in our population and increased with age. Our approach of characterizing large surveys by PreOB/OB and gender ratios appeared promising
MH - Mexico|Distrito Federal
MH - USA
PB - ROCHESTER: NORTH AMER ASSOC STUDY OBESITY
RP - NOT IN FILE
U3 - TC 31
U4 - Endocrinology & Metabolism;Nutrition & Dietetics
U5 - J;Article
AV - English
IS - 1071-7323
UR - ISI:000087403500007
L2 - prevalence;pre-obesity;obesity;national survey;Mexico;Mexican Americans;OVERWEIGHT; EPIDEMIC; TRENDS
SO - Obesity Research 2000 ;8(2):179-185
130
UI - 15837
AU - Arteaga MA
AU - Siciliano B
AD - Univ Nacl Autonoma Mexico, DEPFI, Mexico City 04510, DF, MexicoUniv Naples Federico II, Dipartimento Informat & Sistemist, I-80125 Naples, ItalyArteaga, MA, Univ Nacl Autonoma Mexico, DEPFI, Mexico City 04510, DF, Mexico
TI - On tracking control of flexible robot arms
AB - A controller for solving the tracking problem of flexible robot arms is presented. In order to achieve this goal, the desired trajectory for the link (flexible) coordinates is computed from the dynamic model of the robot arm and is guaranteed to be bounded, and the desired trajectory for the joint (rigid) coordinates can be assigned arbitrarily. The case of no internal damping is also considered, and a robust control technique is used to enhance the damping of the system
MH - Italy
MH - Mexico|Distrito Federal
PB - NEW YORK: IEEE-INST ELECTRICAL ELECTRONICS ENGINEERS INC
RP - NOT IN FILE
U3 - TC 2
U4 - Automation & Control Systems;Engineering, Electrical & Electronic
U5 - J;Article
AV - English
IS - 0018-9286
UR - ISI:000087712300017
L2 - flexible robot arms;nonlinear control;robust control;tracking control;MANIPULATOR ARMS; DYNAMIC-MODEL
SO - Ieee Transactions on Automatic Control 2000 ;45(3):520-527
131
UI - 16099
AU - Arzuffi R
AU - Salinas-Loera C
AU - Racotta IS
AD - Escuela Nacl Ciencias Biol, Inst Politecn Nacl, Dept Fisiol, Mexico City 11340, DF, MexicoCtr Invest Biol Noreste, Div Biol Marina, La Paz, BCS, BoliviaArzuffi, R, IPN, CeProBi, Km 8-5 Carretera,Apto Postal 24, Yautepec 62730, Morelos, Mexico
TI - Food aversion learning induced by lithium chloride in the crayfish Procambarus clarkii
AB - The ability of the crayfish Procambarus clarkii to develop a food aversion learning was examined. For this purpose, in crayfishes fed with trout, a novel food (chicken) was associated in a single trial with a well-known toxic substance, lithium chloride (LiCl), and food intake was recorded for 10 days afterward using a two-choice protocol. All during the experimental period, a significant effect of treatment was observed that accounted for the lower chicken intake in the LiCl-treated group, compared with the control groups (NaCl-treated group and puncture group). In contrast, LiCl-treated animals had an increased trout intake during the entire period. In addition, it was observed that total food intake was similar among the three groups. These results indicate that the crayfish may develop a food aversion learning when illness is induced by LiCl after the animal accepts and eats a novel food. (C) 2000 Elsevier Science Inc. All rights reserved
MH - Bolivia
MH - Mexico|Distrito Federal
MH - Mexico|Morelos
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 2
U4 - Psychology, Biological;Behavioral Sciences
U5 - J;Article
AV - English
IS - 0031-9384
UR - ISI:000086662300007
L2 - food aversion;lithium chloride;crayfish;LOBSTER PANULIRUS-ARGUS
SO - Physiology & Behavior 2000 ;68(5):651-654
132
UI - 15024
AU - Ascencio F
AU - Hirst TR
AU - Wadstrom T
AD - Biol Res Ctr, Marine Pathol Unit, Dept Marine Pathol, La Paz 23000, Baja Calif Sur, MexicoUniv Bristol, Dept Pathol & Microbiol, Bristol BS8 1TH, Avon, EnglandUniv Lund, Dept Med Microbiol, S-22100 Lund, SwedenAscencio, F, Biol Res Ctr, Marine Pathol Unit, Dept Marine Pathol, POB 128, La Paz 23000, Baja Calif Sur, Mexico
TI - Production and secretion of collagen-binding proteins from Aeromonas veronii
AB - Collagen-binding protein (CNBP) synthesized by Aeromonas veronii is located conserved within the subcellular fraction. The results of this study show that 98% of the total CNBP produced by Aer. veronii is present in the extracellular medium, and that the remaining CNBP is distributed either on the cell surface, within the periplasm or anchored on the outer membrane. CNBP is specifically secreted from Aer. veronii into the culture medium, because all the beta -lactamase activity was located in the cells and could be released by polymixin B extraction of periplasmic proteins. CNBP was produced at growth temperatures from 12 degreesC to 42 degreesC, but not at 4 degreesC. The findings indicate that the level of CNBP in the medium increases during the exponential growth phase and reaches a maximum during the early stationary phase. There was less CNBP production in poor nutrient MMB medium than in the rich LB nutrient medium. CNBP secretion, in contrast to aerolysin secretion, was unaffected by the exeA mutation of Aer. hydrophila. It is concluded that CNBP secretion from Aer. veronii must be achieved by a mechanism different from that reported for aerolysin secretion
MH - United Kingdom
MH - Mexico|Baja California Sur
MH - Sweden
PB - OXFORD: BLACKWELL SCIENCE LTD
RP - NOT IN FILE
U3 - TC 2
U4 - Biotechnology & Applied Microbiology;Microbiology
U5 - J;Article
AV - English
IS - 1364-5072
UR - ISI:000089993000008
L2 - EXTRACELLULAR PROTEINS; ESCHERICHIA-COLI; VIBRIO-CHOLERAE; BIOTYPE SOBRIA; HYDROPHILA; FISH; FIBRONECTIN; INFECTIONS; ADHESION; HEMAGGLUTININ
SO - Journal of Applied Microbiology 2000 ;89(4):607-616
133
UI - 16169
AU - Ashtekar A
AU - Corichi A
AD - Penn State Univ, Dept Phys, Ctr Gravitat Phys & Geometry, University Pk, PA 16802, USAUniv Nacl Autonoma Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoUniv Calif Santa Barbara, Inst Theoret Phys, Santa Barbara, CA 93106, USAAshtekar, A, Penn State Univ, Dept Phys, Ctr Gravitat Phys & Geometry, University Pk, PA 16802 USA
TI - Laws governing isolated horizons: inclusion of dilaton couplings
AB - Mechanics of non-rotating black holes was recently generalized by replacing the static evens horizons used in standard treatments with 'isolated horizons'. This framework is extended to incorporate dilaton couplings. Since there can be gravitational and matter radiation outside isolated horizons, now the fundamental parameters of the horizon, used in mechanics, must be defined using only the local structure of the horizon, without reference to infinity. This task is accomplished and the zeroth and first laws are established. To complement the previous work, the entire discussion is formulated tensorially, without any reference to spinors
MH - Mexico|Distrito Federal
MH - USA
PB - BRISTOL: IOP PUBLISHING LTD
RP - NOT IN FILE
U3 - TC 20
U4 - Astronomy & Astrophysics;Physics, Multidisciplinary;Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 0264-9381
UR - ISI:000086502900003
L2 - BLACK-HOLE DYNAMICS; PARTICLE CREATION; THERMODYNAMICS
SO - Classical and Quantum Gravity 2000 ;17(6):1317-1332
134
UI - 16443
AU - Assem I
AU - Liu SP
AU - de la Pena JA
AD - Univ Sherbrooke, Sherbrooke, PQ J1K 2R1, CanadaUniv Nacl Autonoma Mexico, Inst Matemat, Mexico City 04510, DF, MexicoAssem, I, Univ Sherbrooke, Sherbrooke, PQ J1K 2R1, Canada
TI - The strong simple connectedness of a tame tilted algebra
MH - Canada
MH - Mexico|Distrito Federal
PB - NEW YORK: MARCEL DEKKER INC
RP - NOT IN FILE
U3 - TC 3
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0092-7872
UR - ISI:000085637100032
L2 - AUSLANDER-REITEN COMPONENTS
SO - Communications in Algebra 2000 ;28(3):1553-1565
135
UI - 16416
AU - Astey L
AU - Gitler S
AU - Micha E
AU - Pastor G
AD - Inst Politecn Nacl, Ctr Invest, Mexico City 07000, DF, MexicoUniv Rochester, Dept Math, Rochester, NY 14627, USAInst Tecnol Autonoma Mexico, Mexico City 01000, DF, MexicoAstey, L, Inst Politecn Nacl, Ctr Invest, Apartado Postal 14-740, Mexico City 07000, DF, Mexico
TI - Parallelizability of complex projective Stiefel manifolds
AB - The question of parallelizability of the complex projective Stiefel manifolds is settled
MH - Mexico|Distrito Federal
MH - USA
PB - PROVIDENCE: AMER MATHEMATICAL SOC
RP - NOT IN FILE
U3 - TC 0
U4 - Mathematics, Applied;Mathematics
U5 - J;Article
AV - English
IS - 0002-9939
UR - ISI:000085725800040
SO - Proceedings of the American Mathematical Society 2000 ;128(5):1527-1530
136
UI - 15350
AU - Atakishiyev NM
AU - Winternitz P
AD - UNAM, Inst Matemat, Cuernavaca 62210, Morelos, MexicoUniv Montreal, Ctr Rech Math, Montreal, PQ H3C 3J7, CanadaUniv Montreal, Dept Math & Stat, Montreal, PQ H3C 3J7, CanadaAtakishiyev, NM, UNAM, Inst Matemat, Apartado Postal 273-3, Cuernavaca 62210, Morelos, Mexico
TI - Bases for representations of quantum algebras
AB - We derive an explicit expression for the eigenfunctions and the corresponding eigenvalues of the operator [q(1/4)J(+)(q) + q(-1/4) J(-)(q)]q (J3(q)/2) in arbitrary irreducible representation of the algebra su(q) (2). The general form of the intertwining operator A(J) (q), which is a q-extension of the classical su(2)-operator a(J), J(1)a(J) = a(J) J(3), is also found. The matrix elements of A(J) (q) are expressed in terms of the dual q-Kravchuk polynomials
MH - Canada
MH - Mexico|Morelos
PB - BRISTOL: IOP PUBLISHING LTD
RP - NOT IN FILE
U3 - TC 7
U4 - Physics, Multidisciplinary;Physics, Mathematical
U5 - J;Article
AV - English
IS - 0305-4470
UR - ISI:000088933400002
L2 - REAL 2-DIMENSIONAL SPHERE; POLYNOMIALS; SU(Q)(2)
SO - Journal of Physics A-Mathematical and General 2000 ;33(30):5303-5313
137
UI - 14746
AU - Aung H
AU - Toossi Z
AU - McKenna SM
AU - Gogate P
AU - Sierra J
AU - Sada E
AU - Rich EA
AD - Case Western Reserve Univ, Div Infect Dis, Cleveland, OH 44106, USAVet Adm Med Ctr, Cleveland, OH 44106, USANatl Inst Resp Dis, Mexico City, DF, MexicoAung, H, Case Western Reserve Univ, Div Infect Dis, Biomed Res Bldg,Room 1001,10th Floor,10900 Euclid, Cleveland, OH 44106 USA
TI - Expression of transforming growth factor-beta but not tumor necrosis factor-alpha, interferon-gamma, and interleukin-4 in granulomatous lung lesions in tuberculosis
AB - The expression of transforming growth factor (TGF-beta1), tumor necrosis factor-alpha (TNF-alpha), interferon-gamma (IFN-gamma) and interleukin-4 (IL-4) were assessed in lung tissues from patients with tuberculosis. Vimentin, a constitutively expressed cellular protein, was present in 12 of 19 tissue sections indicating adequate preservation of tissue proteins in these cases. Immunohistochemical studies for cytokines were done in the vimentin positive sections only. TGF-beta1 was localized to mononuclear phagocytes of tuberculous lung lesions in 4 of 12 tuberculosis patients. TNF-alpha, IFN-gamma, and IL-4 were absent in sections from all tuberculosis patients. The failure to detect the latter cytokines may indicate that these molecules may not be expressed at the site of disease, or are not a feature of the late stages of tuberculous granulomas. TGF beta -1, although not universally expressed, may be involved in the development and/or consequences of tuberculous granuloma formation. These data substantiate further the role of TGF-beta1 in the immunopathology of tuberculosis, (C) 2000 Harcourt Publishers Ltd
MH - Mexico|Distrito Federal
MH - USA
PB - EDINBURGH: CHURCHILL LIVINGSTONE
RP - NOT IN FILE
U3 - TC 20
U4 - Respiratory System
U5 - J;Article
AV - English
IS - 0962-8479
UR - ISI:000165670700002
L2 - ACTIVE PULMONARY TUBERCULOSIS; INTERMEDIATE-SIZED FILAMENTS; MYCOBACTERIUM-TUBERCULOSIS; CYTOKINE PRODUCTION; LOCAL PRODUCTION; BLOOD MONOCYTES; IFN-GAMMA; FIBROSIS; FACTOR-BETA-1; LOCALIZATION
SO - Tubercle and Lung Disease 2000 ;80(2):61-67
138
UI - 16170
AU - Auria R
AU - Frere G
AU - Morales M
AU - Acuna ME
AU - Revah S
AD - Univ Autonoma Metropolitana Iztapalapa, Dept Chem Engn, Mexico City 09340, DF, MexicoEcole Natl Super Chim, Paris, FranceInst Rech Dev, Mexico City 11530, DF, MexicoRevah, S, Univ Autonoma Metropolitana Iztapalapa, Dept Chem Engn, Apdo Postal 55-534, Mexico City 09340, DF, Mexico
TI - Influence of mixing and water addition on the removal rate of toluene vapors in a biofilter
AB - The effects of successive mixing (homogenization) of packing material (peat), with or without water addition, on the removal of toluene vapors in a biofilter were studied. Over a period of 50 days, an increase in the Elimination Capacity (EC) of approximately 240% was obtained by successive mixing and water additions. After each mixing, a high EC of toluene was maintained only for a short period of 3-4 days. After this time, decreased biofilter performance was observed, probably associated with the development of dried and/or clogged zones. In the long-term experiments, an attenuation of the EC recovery was observed after successive mixing. In this case, an increase of 110% over 4 months of experiment was obtained. The global reduction of EC over time could be explained by the colonization of the biofilter by filamentous fungi which was facilitated by the mixing of the packing material. The most frequently observed fungi were identified as Scedosporium sp, and Cladosporium sp. (C) 2000 John Wiley & Sons, Inc. Biotechnol Bioeng 68: 448-455, 2000
MH - France
MH - Mexico|Distrito Federal
PB - NEW YORK: JOHN WILEY & SONS INC
RP - NOT IN FILE
U3 - TC 30
U4 - Biotechnology & Applied Microbiology
U5 - J;Article
AV - English
IS - 0006-3592
UR - ISI:000086501700010
L2 - mixing;water addition;toluene vapors;fungi;biofilter;DEGRADATION
SO - Biotechnology and Bioengineering 2000 ;68(4):448-455
139
UI - 14506
AU - Avallone S
AU - Guiraud JP
AU - Guyot B
AU - Olguin E
AU - Brillouet JM
AD - Ctr Cooperat Int Rech Agron Dev, Dept FLHOR, F-34032 Montpellier 1, FranceCtr Cooperat Int Rech Agron Dev, Dept CP, F-34032 Montpellier, FranceUniv Sci & Tech Languedoc, Lab Genie Biol & Sci Aliments, F-34095 Montpellier 5, FranceInst Ecol, Xalapa, Veracruz, MexicoBrillouet, JM, Ctr Cooperat Int Rech Agron Dev, Dept FLHOR, BP 5035, F-34032 Montpellier 1, France
TI - Polysaccharide constituents of coffee-bean mucilage
AB - Alcohol-insoluble residues (AIRs) were isolated from hand-dissected and commercial mucilages of depulped coffee beans. Both AIRs had similar polysaccharide composition: pectic substances (about 30%), cellulose (about 8%), and neutral noncellulosic polysaccharides (about 18%). Crude pectins were extracted from AIRs (dry-matter yield: about 23% to 35%) with dilute nitric acid (pH 1.5, 90 degreesC). Both pectins contained about 60% uronic acids with high degree of methyl esterification (about 62%) and moderate degree of acetylation (about 5%). Their molecular weights were low (about 12 to 29 kDa). They did not gel in the presence of sucrose at acidic pH
MH - France
MH - Mexico|Veracruz
PB - CHICAGO: INST FOOD TECHNOLOGISTS
RP - NOT IN FILE
U3 - TC 4
U4 - Food Science & Technology
U5 - J;Article
AV - English
IS - 0022-1147
UR - ISI:000166378300007
L2 - coffee;Coffea arabica L. var. typica Cramer;mucilage;cell-wall polysaccharides;mechanical demucilagination;CELL-WALL POLYSACCHARIDES; QUANTITATIVE-DETERMINATION; PECTINS; EXTRACTION; PULP
SO - Journal of Food Science 2000 ;65(8):1308-1311
140
UI - 14607
AU - Avitia CI
AU - Castellanos-Juarez FX
AU - Sanchez E
AU - Tellez-Valencia A
AU - Fajardo-Cavazos P
AU - Nicholson WL
AU - Pedraza-Reyes M
AD - Univ Guanajuato, Fac Chem, Inst Invest Expt Biol, Guanajuato 36060, MexicoUniv Arizona, Dept Vet Sci & Microbiol, Tucson, AZ, USAPedraza-Reyes, M, Univ Guanajuato, Fac Chem, Inst Invest Expt Biol, POB 187, Guanajuato 36060, Mexico
TI - Temporal secretion of a multicellulolytic system in Myxobacter sp AL-1 - Molecular cloning and heterologous expression of cel9 encoding a modular endocellulase clustered in an operon with cel48, an exocellobiohydrolase gene
AB - Gram-negative soil micro-organism Myxobacter sp. AL-1 possesses at least five extracellular cellulases, the production of which is regulated by the growth cycle. We cloned the complete gene for one of these cellulases, termed cel9, which encoded a 67-kDa modular family 9 endoglycohydrolase, which was produced during the stationary phase of growth and was strongly enhanced by avicel. The predicted product of cel9 matches the structural architecture of family 9 cellulases such as Thermonospora fusca endo/exocellulase E4. Cel9 protein was synthesized in Escherichia coli from a multicopy plasmid and in Bacillus subtilis from the isopropyl thiogalactoside-inducible Pspac promoter and was purified from the culture medium. Thermal stability, optimum pH and temperature dependence of Cel9 were similar when expressed from either source, and were indistinguishable from related cellulases produced by thermophilic bacteria. Downstream from cel9 was found a partial ORF designated cel48, the deduced product of which was highly similar to bacterial exocellobiohydrolases and processive endoglucanases belonging to family 48 of the glycosyl hydrolases. The cel9 and cel48 genes appear to be arranged as part of an operon
MH - Mexico|Guanajuato
MH - USA
PB - OXFORD: BLACKWELL SCIENCE LTD
RP - NOT IN FILE
U3 - TC 10
U4 - Biochemistry & Molecular Biology
U5 - J;Article
AV - English
IS - 0014-2956
UR - ISI:000166113200015
L2 - cellulolytic systems;gene clusters;glycosyl hydrolases;Myxobacter sp AL-1;palindromic DNA sequences;BACILLUS-SUBTILIS; THERMOMONOSPORA-FUSCA; CLOSTRIDIUM-CELLULOLYTICUM; CELLULASE AVICELASE; SEQUENCE-ANALYSIS; ENZYME; ENDOGLUCANASE; FAMILIES; DOMAINS; IDENTIFICATION
SO - European Journal of Biochemistry 2000 ;267(24):7058-7064
141
UI - 16180
AU - Axen GJ
AU - Grove M
AU - Stockli D
AU - Lovera OM
AU - Rothstein DA
AU - Fletcher JM
AU - Farley K
AU - Abbott PL
AD - Univ Calif Los Angeles, Dept Earth & Space Sci, Los Angeles, CA 90095, USAStanford Univ, Dept Geol & Environm Sci, Stanford, CA 94305, USACtr Invest Cient & Educ Super Ensenada, Dept Geol, Ensenada, Baja California, MexicoCALTECH, Div Geol & Planetary Sci, Pasadena, CA 91125, USASan Diego State Univ, Dept Geol Sci, San Diego, CA 92181, USAAxen, GJ, Univ Calif Los Angeles, Dept Earth & Space Sci, Los Angeles, CA 90095 USA
TI - Thermal evolution of Monte Blanco dome: Low-angle normal faulting during Gulf of California rifting and late Eocene denudation of the eastern Peninsular Ranges
MH - USA
MH - Mexico|Baja California
PB - WASHINGTON: AMER GEOPHYSICAL UNION
RP - NOT IN FILE
U3 - TC 11
U4 - Geochemistry & Geophysics
U5 - J;Review
AV - English
IS - 0278-7407
UR - ISI:000086480200001
L2 - NORTHEASTERN BAJA-CALIFORNIA; FISSION-TRACK GEOCHRONOLOGY; LAGUNA-SALADA FAULT; SOUTHERN-CALIFORNIA; UNITED-STATES; SALTON TROUGH; NORTHERN BAJA; OF-CALIFORNIA; PACIFIC PLATE; K-FELDSPAR
SO - Tectonics 2000 ;19(2):197-212
142
UI - 15238
AU - Ayala ME
AU - Ruiz S
AU - Moran MD
AU - Bukovsky A
AU - Dominguez R
AD - UNAM, FES Zaragoza, Biol Reprod Res Unit, Mexico City, DF, MexicoUniv Tennessee, Grad Sch Med, Knoxville, TN, USA
TI - Effects of early postnatal androgenization or estrogenization on the monoamines in the anterior (AH) and medium hypothalamus (MH) of the female rat
MH - Mexico|Distrito Federal
MH - USA
PB - MADISON: SOC STUDY REPRODUCTION
RP - NOT IN FILE
U3 - TC 0
U4 - Reproductive Biology
U5 - J;Meeting Abstract
AV - English
IS - 0006-3363
UR - ISI:000087862300612
SO - Biology of Reproduction 2000 ;62():322-322
143
UI - 16315
AU - Ayala OE
AU - Lardizabal D
AU - Reyes A
AU - Rosales MI
AU - Matutes JA
AU - Arias AG
AD - Univ La Habana, Fac Fis, Dept Fis Aplicada, Havana 10400, CubaCtr Invest Mat Avanzados, Chihuahua 31110, MexicoArias, AG, Univ La Habana, Fac Fis, Dept Fis Aplicada, Havana 10400, Cuba
TI - Vacancy contents in MnZn ferrites from TG curves
AB - Expressions for calculating the cation vacancy contents of MnZn ferrites from thermogravimetric curves are presented together with some experimental data. In a single-phase MnZn ferrite synthesized by conventional ceramic procedures, the O-2 evolution accompanying ferrite formation follows the formal equation. [GRAPHICS] where alpha and beta denote the MnO and ZnO mole fractions in the primary mixture gamma=alpha+beta, theta and phi depend on the quantities of Fe2+ and Mn3+ formed, respectively, phi=theta-phi and sigma'/sigma is a function of the former parameters. Even though the relative amounts of Fe2+/Fe3+ and Mn2+/Mn3+ remain uncertain, the vacancy content [V] of the ferrite can be determined because it depends on phi alone, which is related to the change in mass of the sample as the synthesis takes place through the equation phi=(1.5-gamma)mu(beta)/mu(O2)(1-m(f)/m(i)) Here, m(i) and m(f) are the masses of the sample before and after O-2 evolution, mu(B) is the formula mass of the ferrite and mu(O2) is the O-2 molar mass. Practically vacancy-free single-phase MnZn ferrite samples were obtained by sintering in air at 1250 degrees C and cooling in pure N-2
MH - Cuba
MH - Mexico|Chihuahua
PB - DORDRECHT: KLUWER ACADEMIC PUBL
RP - NOT IN FILE
U3 - TC 3
U4 - Chemistry, Analytical;Chemistry, Physical
U5 - J;Article
AV - English
IS - 1418-2874
UR - ISI:000086006400036
L2 - MnZn ferrite;TG
SO - Journal of Thermal Analysis and Calorimetry 2000 ;59(3):943-949
144
UI - 15371
AU - Ayala S
AU - Noriega-Crespo A
AU - Garnavich PM
AU - Curiel S
AU - Raga AC
AU - Bohm KH
AU - Raymond J
AD - Univ Nacl Autonoma Mexico, Inst Astron, Mexico City 04510, DF, MexicoCALTECH, SIRTF Sci Ctr, IPAC, Pasadena, CA 91125, USAHarvard Smithsonian Ctr Astrophys, Cambridge, MA 02138, USAUniv Washington, Dept Astron, Seattle, WA 98195, USAHarvard Smithsonian Ctr Astrophys, Cambridge, MA 02138, USAAyala, S, Univ Nacl Autonoma Mexico, Inst Astron, Apdo Postal 70-264, Mexico City 04510, DF, Mexico
TI - Optical and near-infrared study of the Cepheus E outflow, a very low-excitation object
AB - We present images and spectra of the Cepheus E (Cep E) region at both optical and infrared wavelengths. Only the brightest region of the southern lobe of the Cep E outflow reveals optical emission, suggesting that the extinction close to the outflow source plays an important role in the observed difference between the optical and IR morphologies. Cep E is a unique object since it provides a link between the spectroscopic properties of the optical Herbig-Haro (HH) objects and those of deeply embedded outflows. The observed H-2 infrared lines allow us to determine an excitation temperature of similar to 2300 K, an Ortho-to-Para ratio of similar to 3, and an H-2 (1, 0)/(2, 1) S(1) line ratio of similar to 9. These results are consistent with the values observed for WH objects with detected NIR emission lines, with shock excitation as the main mechanism for their formation, and also with the values observed for embedded, NIR flows. The optical spectroscopic characteristics of Cep E (HH 377) appear to be similar to the ones of low-excitation HH objects. However, the electron density determined from the CS nl lambda lambda 6731/6717 line ratio for this object (n(e) = 4100 cm(-3)), and the [O I] lambda 6300/H alpha, [S II] lambda lambda(6717 + 6731)/H alpha ratios are higher than the values of all of the previously studied low-excitation HH objects. This result is likely to be the consequence of an anomalously high environmental density in the HH 377 outflow. The ionization fraction obtained for HH 377 is x(e) similar to 1%. From this result, together with the observed [O I] lambda 6300/H alpha line ratio, we conclude that the observed H alpha line emission is collisionally excited. From a comparison with shock models, we also conclude that the extinction toward HH 377 is very low. Comparing the observed H beta and H alpha fluxes of HH 377 with model predictions, we determine a shock speed between 15 and 20 km s(-1), although somewhat higher velocities also produce spectra with line ratios that qualitatively agree with the observations of HH 377
MH - Mexico|Distrito Federal
MH - USA
PB - CHICAGO: UNIV CHICAGO PRESS
RP - NOT IN FILE
U3 - TC 5
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-6256
UR - ISI:000089040800032
L2 - infrared radiation;ISM : individual (Cepheus E, HH 377);ISM : jets and outflows;HERBIG-HARO OBJECTS; MOLECULAR-HYDROGEN; CEP-E; H-2 FLUORESCENCE; EMISSION; SHOCK; JETS; SPECTROSCOPY; IONIZATION; EXTINCTION
SO - Astronomical Journal 2000 ;120(2):909-919
145
UI - 15441
AU - az-Arencibia P
AU - Hernandez-Calderon I
AU - Hernandez-Ramirez LM
AU - Tamargo MC
AD - CINVESTAV, Dept Phys, Mexico City 07000, DF, MexicoCUNY City Coll, Dept Chem, New York, NY 10031, USAHernandez-Ramirez, LM, CINVESTAV, Dept Phys, Apdo Postal 14-740, Mexico City 07000, DF, Mexico
TI - A two-level model for intra-well exciton migration in Zn1-xCdxSe quantum wells
AB - In this work we present a simple two-level model, which can be employed to describe the migration of weakly localized excitons in quantum wells (QW). The migration of excitons is an intra-well process which can be readily observed in QWs which present thickness fluctuations of a few monolayers that extend over large area terraces (also called islands) with dimensions much larger than the Bohr radius of the exciton. This effect is experimentally observed as relative changes of the intensity of the spontaneous emission, as a function of temperature, of the transitions of QWs with different thickness. This model has been successfully applied to the analysis of the temperature dependence of the photoluminescence spectra of Zn1-xCdxSe QWs
MH - Mexico|Distrito Federal
MH - USA
PB - BERLIN: WILEY-V C H VERLAG GMBH
RP - NOT IN FILE
U3 - TC 3
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0370-1972
UR - ISI:000088768800006
L2 - RECOMBINATION; SPECTROSCOPY; LOCALIZATION; CARRIERS; DYNAMICS; STATES; LASERS
SO - Physica Status Solidi B-Basic Research 2000 ;220(1):27-31
146
UI - 15820
AU - az-Arencibia P
AU - Hernandez-Calderon I
AU - Hernandez-Ramirez LM
AU - Tamargo MC
AD - CINVESTAV, Dept Phys, Mexico City 07000, DF, MexicoCUNY City Coll, Dept Chem, New York, NY 10031, USAUniv Havana, Fac Phys, Havana, CubaHernandez-Calderon, I, CINVESTAV, Dept Phys, Apdo Postal 14-470, Mexico City 07000, DF, Mexico
TI - Photoluminescence properties of intra-well exciton migration in Zn1-xCdxSe quantum wells
AB - We report the results of the investigation of the temperature dependence and the nature of the spontaneous excitonic emission of Zn1-xCdxSe QWs. The spectra are dominated by two main peaks, which show a strong change in relative intensities with temperature. The presence in the spectra of biexcitons and bound excitons was ruled out after the corresponding analyses. Calculation of the fundamental transitions of the QWs indicated that the peaks were due to thickness fluctuations of 1 and 2 monomolecular layers. The changes in the relative intensities of the two peaks in the photoluminescence spectra with temperature are attributed to exciton migration between QW regions differing in thickness one or two monomolecular layers (ML). The measured activation energy necessary for exciton migration, in order to establish thermal equilibrium as temperature increases, coincides with the energy difference of the exciton ground state of QWs with 1-2 ML thickness difference. The successful analysis of the spectra in terms of a simple two-level model indicated that localization of excitons due to QW thickness fluctuations and exciton migration are basic processes which have strong influence in the temperature dependence of the spontaneous emission of Zn1-xCdxSe QWs. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Cuba
MH - Mexico|Distrito Federal
MH - USA
PB - OXFORD: ELSEVIER ADVANCED TECHNOLOGY
RP - NOT IN FILE
U3 - TC 1
U4 - Engineering, Electrical & Electronic;Nanoscience & Nanotechnology
U5 - J;Article
AV - English
IS - 0026-2692
UR - ISI:000087737600009
L2 - photoluminescence;exciton;quantum well;STIMULATED-EMISSION; OPTICAL-PROPERTIES; ROOM-TEMPERATURE; RECOMBINATION; LOCALIZATION; DYNAMICS; LASERS; HETEROSTRUCTURES; SPECTROSCOPY; CARRIERS
SO - Microelectronics Journal 2000 ;31(6):443-450
147
UI - 15823
AU - az-Arencibia P
AU - Hernandez-Calderon I
AU - Hernandez-Ramirez LM
AU - Tamargo MC
AD - CINVESTAV, Dept Phys, Mexico City 07000, DF, MexicoCUNY City Coll, Dept Chem, New York, NY 10031, USADiaz-Arencibia, P, Univ Havana, Fac Phys, Havana, Cuba
TI - Temperature dependence of exciton localization in Zn1-xCdxSe quantum wells
AB - We report the results of the investigation of the temperature dependence of the spontaneous emission of localized excitons in Zn1-xCdxSe quantum wells (QWs). Two main peaks, which show a strong change in relative intensities with temperature, dominate the spectra, The presence in the spectra of biexcitons and bound excitons was ruled out after the corresponding analyses. Calculation of the fundamental transitions of the QWs suggested that the peaks are due to thickness fluctuations of one and two monomolecular layers. The successful analysis of the spectra in terms of a simple two-level model indicated that localization of excitons due to QW thickness fluctuations and exciton migration are basic processes which have noticeable;influence in the spontaneous emission of Zn1-xCdxSe QWs. (C) 2000 American Vacuum Society
MH - Cuba
MH - Mexico|Distrito Federal
MH - USA
PB - MELVILLE: AMER INST PHYSICS
RP - NOT IN FILE
U3 - TC 4
U4 - Engineering, Electrical & Electronic;Nanoscience & Nanotechnology;Physics, Applied
U5 - J;Article
AV - English
IS - 1071-1023
UR - ISI:000087654200076
L2 - RECOMBINATION; SPECTROSCOPY; CARRIERS; DYNAMICS; STATES; LASERS
SO - Journal of Vacuum Science & Technology B 2000 ;18(3):1526-1529
148
UI - 14729
AU - az-Calleja R
AU - Garcia-Bernabe A
AU - Sanchis MJ
AU - del Castillo LF
AD - Univ Politecn Valencia, Dept Termodinam Aplicada, E-46071 Valencia, SpainUniv Nacl Autonoma Mexico, Inst Invest Mat, Mexico City 04510, DF, MexicoDiaz-Calleja, R, Univ Politecn Valencia, Dept Termodinam Aplicada, E-46071 Valencia, Spain
TI - Memory function for dielectric relaxation
AB - The second-order memory function (SOMF) for the dicyclohexylmetyl-2metyl succinate is obtained by using simple numerical manipulation of the experimental dielectric data. According to the prescription given in a previous paper [J. Chem. Phys. 109, 9057 (1998)], the frequency behavior of the real and imaginary parts of the SOMF is discussed in terms of the Havriliak-Negami equation of the dielectric function, and together with the three-variable model describing the evolution of the torque-autocorrelation function. Furthermore, in this paper we present the temperature dependence of the parameters, which characterize the SOMF behavior for two ester substances. (C) 2000 American Institute of Physics. [S0021- 9606(00)51048-4]
MH - Mexico|Distrito Federal
MH - Spain
PB - MELVILLE: AMER INST PHYSICS
RP - NOT IN FILE
U3 - TC 2
U4 - Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 0021-9606
UR - ISI:000165841300044
L2 - LIQUIDS; WATER
SO - Journal of Chemical Physics 2000 ;113(24):11258-11263
149
UI - 15109
AU - az-Cruz JL
AU - Hernandez JM
AU - Toscano JJ
AD - BUAP, Inst Fis, Puebla 72500, MexicoUniv Calif Riverside, Dept Phys, Riverside, CA 92521, USABUAP, Fac Ciencias Fis Matemat, Puebla 72000, MexicoDiaz-Cruz, JL, BUAP, Inst Fis, Ap Postal J-48, Puebla 72500, Mexico
TI - Impact of the bounds on Higgs mass and m(w) on effective theories
AB - We study the inter-relations that exist between the present experimental bounds on the Higgs mass, as obtained from radiative corrections to m(W), and the effective parameters, alpha(i) and Lambda. We find that the SM bounds on m(H), arising from a precise determination of the W mass, can be substantially modified by the presence of dimension-six operators which appear in the linear realization of the effective Lagrangian approach. A Higgs mass as heavy as 700 GeV can be allowed for scales of new physics of the order of 1 TeV
MH - Mexico|Puebla
MH - USA
PB - SINGAPORE: WORLD SCIENTIFIC PUBL CO PTE LTD
RP - NOT IN FILE
U3 - TC 1
U4 - Physics, Nuclear;Physics, Particles & Fields;Physics, Mathematical
U5 - J;Article
AV - English
IS - 0217-7323
UR - ISI:000089631700005
L2 - STANDARD MODEL; VECTOR BOSONS; COUPLINGS
SO - Modern Physics Letters A 2000 ;15(21):1377-1384
150
UI - 15507
AU - az-Gomez O
AU - Rodriguez JC
AU - Shelton AM
AU - Lagunes T
AU - Bujanos M
AD - Univ Autonoma San Luis Potosi, Fac Agron, San Luis Potosi 78000, MexicoColegio Postgrad, Inst Fitosanidad, Texcoco 56230, Estado Mexico, MexicoCornell Univ, New York State Agr Expt Stn, Dept Entomol, Geneva, NY 14456, USACampo Expt Bajio, Celaya, Gto, MexicoDiaz-Gomez, O, Univ Autonoma San Luis Potosi, Fac Agron, Alvaro Obregon 64, San Luis Potosi 78000, Mexico
TI - Susceptibility of Plutella xylostella (L.) (Lepidoptera : Plutellidae) populations in Mexico to commercial formulations of Bacillus thuringiensis
AB - Populations of diamondback moth, Plutella xylostella (L.), sampled from commercial fields of crucifers in three states of Mexico, were tested for susceptibility to commercial formulations of Bacillus thuringiensis subsp. kurstaki (Berliner) (Dipel 2X), B. thuringiensis subsp. aizawai (XenTari), delta endotoxin Cry 1C (MC), and CryIA(c) (MW), and a mixture of B. thuringiensis subsp. kurstaki and subsp. aizawai (Agree). Leaf-dip bioassays confirmed variation in susceptibility of up to 13-fold for MVP, 12-fold for Dipel 2X, sevenfold for XenTari, fivefold for Agree, and less than fivefold for MC. Comparisons with previously published data indicate that at least the 12-fold variation in Dipel 2X would result in significant differences in control in the field. Based on the LC99 values observed for the products, we propose discriminating concentrations far each product. To ensure continued performance in the field we suggest that a resistance monitoring program be implemented to detect any changes in susceptibility to B. thuringiensis products and specific toxins and that their use be restricted to one generation per crop and that they be rotated with other groups of insecticides. Furthermore, we suggest enforcement of a crucifer host-free period and the development and implementation of cultural and biological control strategies to reduce overall population pressure so that fewer insecticidal treatments will be needed
MH - Mexico|Estado De Mexico
MH - Mexico|Guanajuato
MH - Mexico|San Luis Potosi
MH - USA
PB - LANHAM: ENTOMOL SOC AMER
RP - NOT IN FILE
U3 - TC 8
U4 - Entomology
U5 - J;Article
AV - English
IS - 0022-0493
UR - ISI:000088599000060
L2 - Plutella xylostella;Bacillus thuringiensis;resistance;DIAMONDBACK MOTH LEPIDOPTERA; INSECTICIDE RESISTANCE; CRYSTAL PROTEIN; EVOLUTION; PYRALIDAE; AMERICA; FIELD
SO - Journal of Economic Entomology 2000 ;93(3):963-970
151
UI - 15453
AU - az-Ortiz A
AU - Sanchez JM
AU - Moran-Lopez JL
AD - Univ Texas, Texas Mat Inst, Austin, TX 78712, USAUniv Autonoma San Luis Potosi, Inst Fis, San Luis Potosi 78000, SLP, MexicoDiaz-Ortiz, A, Univ Texas, Texas Mat Inst, Austin, TX 78712, USA
TI - Phase transitions in confined antiferromagnets
AB - Confinement effects on the phase transitions in antiferromagnets are studied as a function of the surface coupling v and the surface field h for b.c.c.(110) films. Unusual topologies for the phase diagram are attained for particular combinations of v and h. It is shown that some of the characteristics of the finite-temperature behavior of the system are driven by its low-temperature properties and consequently can be explained in terms of a ground-state analysis. Cluster variation free energies are used for the investigation of the finite temperature behavior
MH - Mexico|San Luis Potosi
MH - USA
PB - BERLIN: WILEY-V C H VERLAG GMBH
RP - NOT IN FILE
U3 - TC 1
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0370-1972
UR - ISI:000088768800069
L2 - SURFACE SPIN-FLOP; CRITICAL-BEHAVIOR; BINARY-ALLOYS; SUPERLATTICES; FILMS; FE/CR(211); FLUIDS; MODEL
SO - Physica Status Solidi B-Basic Research 2000 ;220(1):389-394
152
UI - 16304
AU - az-Perez JC
AU - Bautista S
AU - Villanueva R
AD - Univ Georgia, Coastal Plain Expt Stn, Dept Hort, Tifton, GA 31793, USANatl Polytech Inst, Ctr Dev Biot Prod, Dept Biotechnol, Yautepec 62730, Morelos, MexicoDiaz-Perez, JC, Univ Georgia, Coastal Plain Expt Stn, Dept Hort, Tifton Campus, Tifton, GA 31793 USA
TI - Quality changes in sapote mamey fruit during ripening and storage
AB - Physical and chemical changes in sapote mamey (Pouteria sapota (Jacq.) H.E. Moore and Steam) fruit during ripening and storage at various temperatures were evaluated. Ripening was associated with flesh softening, an increase in soluble solids content (SSC), and a change in flesh color from yellow or pale pink to a dark pink or red. No changes in fruit skin color or in flesh acidity were observed as ripening progressed. Ripe fruit had 30% or higher SSC, orange or red flesh (hue angle = 52; chroma = 45; L = 60), acidity of 6-8 mM H+, and flesh firmness (compression force) less than or equal to 50 N. Flesh turned brown (L* value declined) in overripe fruit. Fruit held at 27, 25, or 20 degrees C ripened in 3.5, 5 or 7 days after harvest, respectively. Fruit kept at 10 degrees C showed minor changes in color and firmness and a slow rate of SSC increase. Fruit stored at 10 or 15 degrees C and then ripened at 20 degrees C had portions of the flesh with a much higher firmness and poorer development of red color compared to other parts of the fruit. This uneven ripening was probably a result of chilling injury. The number of fruit with injury was higher at 10 degrees C than at 15 degrees C, and increased with storage time. The rates of fruit weight loss relative to the initial fruit weight were 0.58, 0.98 and 1.83% d(-1) at 10, 20 and 27 degrees C, respectively. (C) 2000 Elsevier Science B.V. All rights reserved
MH - USA
MH - Mexico|Morelos
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 9
U4 - Agronomy;Food Science & Technology;Horticulture
U5 - J;Article
AV - English
IS - 0925-5214
UR - ISI:000086110400009
L2 - chilling injury;postharvest;quality;ripening;fruit transpiration;Pouteria sapota
SO - Postharvest Biology and Technology 2000 ;18(1):67-73
153
UI - 15206
AU - Bada JL
AU - Lazcano A
AD - Univ Calif San Diego, Scripps Inst Oceanog, La Jolla, CA 92093, USAUNAM, Fac Ciencias, Dept Biol, Mexico City, DF, MexicoBada, JL, Univ Calif San Diego, Scripps Inst Oceanog, La Jolla, CA 92093 USA
TI - Stanley Miller's 70th birthday
MH - USA
MH - Mexico|Distrito Federal
PB - DORDRECHT: KLUWER ACADEMIC PUBL
RP - NOT IN FILE
U3 - TC 3
U4 - Biology
U5 - J;Biographical-Item
AV - English
IS - 0169-6149
UR - ISI:000089355900001
SO - Origins of Life and Evolution of the Biosphere 2000 ;30(2-4):107-112
154
UI - 15990
AU - Baier G
AU - Leder RS
AU - Parmananda P
AD - Univ Autonoma Morelos, Fac Ciencias, Cuernavaca, Morelos, MexicoUniv Autonoma Morelos, Fac Med, Cuernavaca, Morelos, MexicoUniv Wisconsin, Dept Elect Engn, Madison, WI 53706, USABaier, G, Univ Autonoma Morelos, Fac Ciencias, Cuernavaca, Morelos, Mexico
TI - Human electroencephalogram induces transient coherence in excitable spatiotemporal chaos
AB - A time series from a human electroencephalogram (EEG) is used as a local perturbation to a reaction diffusion model with spatiotemporal chaos. For certain finite ranges of amplitude and frequency it is observed that the strongly irregular perturbations can induce transient coherence in the chaotic system. This could be interpreted as "on-line" detection of an inherently correlated pattern embedded in the EEG
MH - Mexico|Morelos
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 5
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0031-9007
UR - ISI:000086941600062
L2 - CHEMICAL TURBULENCE; EPILEPTIC SEIZURES; DISORDER; PATTERNS; NOISE
SO - Physical Review Letters 2000 ;84(19):4501-4504
155
UI - 15960
AU - Balda MS
AU - Flores-Maldonado C
AU - Cereijido M
AU - Matter K
AD - Univ Geneva, Dept Biol Cellulaire, CH-1211 Geneva 4, SwitzerlandCtr Res & Adv Studies, Dept Physiol, Mexico City 07300, DF, MexicoMatter, K, Univ Geneva, Dept Biol Cellulaire, 30 Quai Ernest Ansermet, CH-1211 Geneva 4, Switzerland
TI - Multiple domains of occludin are involved in the regulation of paracellular permeability
AB - Tight junctions form selective paracellular diffusion barriers that regulate the diffusion of solutes across epithelia and constitute intramembrane diffusion barriers that prevent the intermixing of apical and basolateral lipids in the extracytoplasmic leaflet of the plasma membrane. In MDCK cells, previous expression experiments demonstrated that occludin, a tight junction protein with four transmembrane domains, is critically involved in both of these tight junction functions and that its COOH-terminal cytoplasmic domain is of functional importance. By expressing mutant and chimeric occludin that exert a dominant negative effect on selective paracellular diffusion, we now demonstrate that the extracytoplasmic domains and at least one of the transmembrane domains are also critically involved in selective paracellular permeability. Multiple domains of occludin are thus important For the regulation of paracellular permeability, Expression of chimeras containing at least one transmembrane domain of occludin also resulted in an enhanced intracellular accumulation of claudin-4, another transmembrane protein of tight junctions, suggesting that the two proteins may cooperate in the regulation of paracellular permeability. (C) 2000 Wiley-Liss, Inc
MH - Mexico|Distrito Federal
MH - Switzerland
PB - NEW YORK: WILEY-LISS
RP - NOT IN FILE
U3 - TC 47
U4 - Biochemistry & Molecular Biology;Cell Biology
U5 - J;Article
AV - English
IS - 0730-2312
UR - ISI:000087216100008
L2 - occludin;paracellular permeability;claudins;TIGHT-JUNCTION STRUCTURE; INTEGRAL MEMBRANE-PROTEINS; CANINE KIDNEY-CELLS; MOUSE MACROPHAGE; BARRIER; RESISTANCE; TRANSPORT; STRANDS; FIBROBLASTS; COMPONENT
SO - Journal of Cellular Biochemistry 2000 ;78(1):85-96
156
UI - 16475
AU - Ballote LD
AU - Ramanauskas R
AU - Bartolo-Perez P
AD - CINVESTAV, IPN, Unidad Merida, Merida 97310, Yuc, VenezuelaCICATA IPN, Mexico City 22800, DF, MexicoBallote, LD, CINVESTAV, IPN, Unidad Merida, Apdo Postal 73 Cordemex, Merida 97310, Yuc, Venezuela
TI - Mn oxide film as corrosion inhibitor of Zn-Mn coatings
AB - Despite the technological relevance of galvanized steels, in past years not enough attempts have been made to improve the corrosion resistance of hot dip galvanizing Zn coatings by alloying. In the present work a Zn-0.5%Mn coating was produced under controlled laboratory conditions. The level of corrosion protection offered by the addition of Mn to the Zn coating was investigated. Polarization measurements in sodium chloride solution and x-ray diffraction were used to determine their corrosion behavior. The corrosion rates of Zn and Zn-0.5%Mn coatings were in the same order of magnitude. However by comparing the corrosion rate on several samples, a reduction of the corrosion rate of the samples containing Mn was observed. This result was attributed to the presence of an oxide manganese film on the surface coating. This film was studied by AES and XPS spectroscopies. Preliminary results are presented in this paper
MH - Mexico|Distrito Federal
MH - Venezuela
PB - LONDON: FREUND PUBLISHING HOUSE LTD
RP - NOT IN FILE
U3 - TC 2
U4 - Electrochemistry;Metallurgy & Metallurgical Engineering;Materials Science, Coatings & Films
U5 - J;Article
AV - English
IS - 0048-7538
UR - ISI:000085452300004
L2 - hot-dip galvanizing;corrosion resistance;manganese;sodium chloride;zinc;auger electron spectroscopy;x-ray photoelectron spectroscopy;ZINC; CHLORIDE; STEEL
SO - Corrosion Reviews 2000 ;18(1):41-51
157
UI - 15252
AU - Baltazar U
AU - Dunn J
AU - Gonzalez-Diaz S
AU - Browder W
AD - Hosp Gen Ciudad Mexico SSA, Dept Surg, Mexico City, DF, MexicoDunn, J, E Tennessee State Univ, James H Quillen Coll Med, Dept Surg, Box 70575, Johnson City, TN 37614 USA
TI - Agenesis of the gallbladder
AB - Agenesis of the gallbladder is rare. Three groups have been identified: these with multiple fetal anomalies, asymptomatic cases, and symptomatic cases. Right upper quadrant pain is present in 90% of the cases, nausea and vomiting in 60%, and jaundice in 35%, Operative strategy is aimed at thorough exploration to locate an aberrant gallbladder, We treated a 72-year-old woman with right upper quadrant pain, nausea, and vomiting but no fever or jaundice. Physical examination revealed right upper quadrant tenderness without rebound. The white blood cell count was 10,300/mm(3), Total bilirubin level was 1.6 mg/dL. Ultrasonography revealed one gallstone and an enlarged common bile duct. Laparoscopic cholecystectomy was converted to open technique after failure to locate the gallbladder, On intraoperative cholangiogram, no gallbladder was identified. A T-tube was placed
MH - Mexico|Distrito Federal
MH - USA
PB - BIRMINGHAM: SOUTHERN MEDICAL ASSN
RP - NOT IN FILE
U3 - TC 7
U4 - Medicine, General & Internal
U5 - J;Article
AV - English
IS - 0038-4348
UR - ISI:000089274800016
SO - Southern Medical Journal 2000 ;93(9):914-915
158
UI - 16296
AU - Bang JM
AU - Mazur AI
AU - Shirokov AM
AU - Smirnov YF
AU - Zaytsev SA
AD - Univ Copenhagen, Niels Bohr Inst, DK-2100 Copenhagen 0, DenmarkKhabarovsk State Tech Univ, Dept Phys, Khabarovsk 680035, RussiaMoscow MV Lomonosov State Univ, Skobeltsyn Inst Nucl Phys, Moscow 119899, RussiaIowa State Univ, Int Inst Theoret & Appl Phys, Ames, IA 50011, USANatl Autonomous Univ Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoBang, JM, Univ Copenhagen, Niels Bohr Inst, Blegdamsvej 17, DK-2100 Copenhagen 0, Denmark
TI - P-matrix and J-matrix approaches: Coulomb asymptotics in the harmonic oscillator representation of scattering theory
AB - The relation between the R- and P-matrix approaches and the harmonic oscillator representation of the quantum scattering theory (J-matrix method) is discussed. We construct a discrete analogue of the P-matrix that is shown to be equivalent to the usual P-matrix in the quasiclassical limit. A definition of the natural channel radius is introduced. As a result, it is shown to be possible to use a well-developed technique of R- and P-matrix theory for calculation of resonant states characteristics. scattering phase shifts, etc., in the approaches based on harmonic oscillator expansions, e.g., in nuclear shell-model calculations. The P-matrix is used also for formulation of the method of treating Coulomb asymptotics in the scattering theory in oscillator representation. (C) 2000 Academic Press
MH - Denmark
MH - Mexico|Distrito Federal
MH - Russia
MH - USA
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 6
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0003-4916
UR - ISI:000086173400003
L2 - ELECTRON-HYDROGEN SCATTERING; NUCLEON-NUCLEON-SCATTERING; CONTINUUM RPA; MODEL; RESONANCES; EXPANSIONS; MOMENTUM; DECAY
SO - Annals of Physics 2000 ;280(2):299-335
159
UI - 16063
AU - Barats MS
AU - Gonick HC
AU - Rothenberg S
AU - Balabanian M
AU - Manton WI
AD - Cedars Sinai Med Ctr, Div Nephrol, Los Angeles, CA 90048, USACedars Sinai Med Ctr, Allen Res Inst, Dept Med, Div Nephrol, Los Angeles, CA 90048, USAUniv Calif Los Angeles, Los Angeles, CA, USACharles R Drew Univ Med & Sci, Environm Res Ctr, Dept Anesthesiol, Los Angeles, CA 90059, USANatl Inst Publ Hlth, Ctr Study Populat Hlth, Cuernavaca, Morelos, MexicoKidney Consultants Med Grp, Mission Hills, CA, USAUniv Texas, Dept Geosci, Richardson, TX, USAGonick, HC, Cedars Sinai Med Ctr, Div Nephrol, Becker Bldg,Room 227,8700 Beverly Blvd, Los Angeles, CA 90048 USA
TI - Severe lead-induced peripheral neuropathy in a dialysis patient
AB - Toxic neuropathy caused by lead (manifested as wrist drop) was a frequent phenomenon before 1925, In modern times, it is a distinct rarity, We report herein a Hispanic woman who developed end-stage renal failure, followed by wrist drop, in whom the maximal total blood lead was 69 mu g/dL. Measurements of lead in her tibia and calcaneus by K-x-ray fluorescence, however, showed markedly elevated values, The wrist drop cleared after four treatments with intravenous calcium sodium edetate (Ca EDTA), In vitro studies of Pb-210 uptake by red blood cells (RBC) after incubation with normal or uremic plasma indicated that Pb-210 uptake was inhibited by uremic plasma, These studies suggest the presence of a transport inhibitor in uremia that modifies the distribution of lead between plasma and RBC, leading to lower overall blood values. (C) 2000 by the National Kidney Foundation, Inc
MH - USA
MH - Mexico|Morelos
PB - PHILADELPHIA: W B SAUNDERS CO
RP - NOT IN FILE
U3 - TC 1
U4 - Urology & Nephrology
U5 - J;Article
AV - English
IS - 0272-6386
UR - ISI:000086908200028
L2 - lead;neuropathy;dialysis;active transport;CUMULATIVE EXPOSURE; SMELTER WORKERS; WHOLE-BLOOD; BONE; PLASMA; HYPERTENSION; INDICATORS; CHILDREN; DISEASE
SO - American Journal of Kidney Diseases 2000 ;35(5):963-968
160
UI - 16272
AU - Barbarin-Castillo JM
AU - Soto-Regalado E
AU - Mclure IA
AD - Univ Nuevo Leon, Fac Ciencias Quim, Monterrey, NL, MexicoUniv Sheffield, Dept Chem, Sheffield S3 7HF, S Yorkshire, EnglandBarbarin-Castillo, JM, Univ Nuevo Leon, Fac Ciencias Quim, Monterrey, NL, Mexico
TI - A test of the McGlashan and Potter correlation for second virial coefficients of mixtures containing a tetramethyl substance
AB - The corresponding states correlation of McGlashan and Potter has been tested twice in order to to predict the second virial coefficients of the mixtures (methane + tetramethylsilane or 2.2-dimethylpropane) at four different compositions in the temperature ranges 303.16 K to 403.16 K and 323.16 K to 403.16 K, repsectively. Predicted values are essentially identical to those obtained by using the more tested correlation of Pitzer-Curl-Tsonopoulos. Predictions were improved significantly, to yield deviations of only (0 to 2) per cent, after correcting the pseudocritical temperature by an empirical device due to Gunn and Prausnitz. (C) 2000 Academic Press
MH - United Kingdom
MH - Mexico|Nuevo Leon
PB - LONDON: ACADEMIC PRESS LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Thermodynamics;Chemistry, Physical
U5 - J;Article
AV - English
IS - 0021-9614
UR - ISI:000086215800011
L2 - corresponding states correlations;second virial coefficients;mixtures;tetramethylsilane;2,2-dimethylpropane;methane
SO - Journal of Chemical Thermodynamics 2000 ;32(4):567-569
161
UI - 15646
AU - Barbour MM
AU - Fischer RA
AU - Sayre KD
AU - Farquhar GD
AD - Australian Natl Univ, Inst Adv Studies, Res Sch Biol Sci, Environm Biol Grp, Canberra, ACT 2601, AustraliaAustralian Ctr Int Agr Res, Canberra, ACT 2601, AustraliaCIMMYT, Mexico City 06600, DF, MexicoFarquhar, GD, Australian Natl Univ, Inst Adv Studies, Res Sch Biol Sci, Environm Biol Grp, GPO Box 475, Canberra, ACT 2601, Australia
TI - Oxygen isotope ratio of leaf and grain material correlates with stomatal conductance and grain yield in irrigated wheat
AB - Theory (Craig and Gordon 1965; Dongmann et al. 1974; Sternberg et al. 1986; Farquhar and Lloyd 1993) suggests that the oxygen isotope ratio (delta(18)O) of plant material should reflect the evaporative conditions under which the material was formed, so that differences in stomatal conductance should show up in plant delta(18)O. To test this theory we measured the oxygen isotope ratio of organic matter from flag leaves at anthesis and grain at harvest from eight cultivars of spring wheat (Triticum aestivum L.) grown under irrigation in each of three seasons in Mexico. The cultivars ranged widely in stomatal conductance and in average grain yield, with which conductance was positively correlated. Supporting theory, the oxygen isotope ratio of flag leaves (delta(18)O(l)) was found to correlate negatively with stomatal conductance for two of the three seasons. The significant correlations are consistent with high conductance cultivars having lower leaf temperatures and kinetic fractionation factors, and higher vapour pressure fractionation factors and Peclet numbers, all of which combine to result in less enriched delta(18)O(l). Yield (grain weight per square meter) was also found to be significantly negatively correlated with delta(18)O(l) in two of the three seasons. delta(18)O(l) was as good a predictor of yield as stomatal conductance, and significantly better than carbon isotope discrimination. Correlations between grain delta(18)O (delta(18)O(g)) and physiological parameters were less clear. Significant negative correlations between delta(18)O(g) and stomatal conductance, leaf temperature and yield were found only during the first season. By measuring the oxygen isotope ratio of cellulose extracted from leaf samples, the difference in fractionation factors (epsilon(cp)) for cellulose and whole leaf tissue was assessed. epsilon(cp) was found to be variable, and more negative when delta(18)O(c) and delta(18)O(l) were lower. Cultivar means for delta(13)C and delta(18)O of whole leaf material were found to be significantly positively related, and the factors required to produce such a relationship are discussed
MH - Australia
MH - Mexico|Distrito Federal
PB - COLLINGWOOD: C S I R O PUBLISHING
RP - NOT IN FILE
U3 - TC 38
U4 - Plant Sciences
U5 - J;Article
AV - English
IS - 0310-7841
UR - ISI:000088166400001
L2 - PHOTOSYNTHETIC RATE; PIMA COTTON; CELLULOSE; WATER; DISCRIMINATION; FRACTIONATION; TEMPERATURE; DELTA-C-13; DELTA-O-18; PROGRESS
SO - Australian Journal of Plant Physiology 2000 ;27(7):625-637
162
UI - 15462
AU - Barmenkov YO
AU - Kir'yanov AV
AU - Starodumov AN
AU - Maslyanitsyn IA
AU - Shigorin VD
AU - Lemmetyinen H
AD - Ctr Invest Opt, Leon, Guanajuato, MexicoRussian Acad Sci, Inst Gen Phys, Moscow, RussiaTampere Univ Technol, Inst Mat Chem, FIN-33101 Tampere, FinlandBarmenkov, YO, Ctr Invest Opt, Loma Bosque 115, Leon, Guanajuato, Mexico
TI - Study of nonlinear optical properties of multilayer Langmuir-Blodgett films containing bacteriorhodopsin
AB - Multilayer oriented Langmuir-Blodgett films of bacteriorhodopsin were prepared and their nonlinear optical properties, including second harmonic generation and photoresponse at a two phase-modulated beams mixing, were Investigated. The nonlinear component of refractive index of the films was measured
MH - Finland
MH - Mexico|Guanajuato
MH - Russia
PB - AUGUSTA: AMER SOC PHOTOBIOLOGY
RP - NOT IN FILE
U3 - TC 0
U4 - Biochemistry & Molecular Biology;Biophysics
U5 - J;Article
AV - English
IS - 0031-8655
UR - ISI:000088789400001
L2 - PURPLE MEMBRANE; TIME; HOLOGRAPHY; PHASE
SO - Photochemistry and Photobiology 2000 ;72(2):151-154
163
UI - 16293
AU - Barmenkov YO
AU - Kir'yanov AV
AU - Starodumov AN
AU - Kozhevnikov NM
AU - Lemmetyinen H
AD - Ctr Invest Opt, Leon 37150, Gto, MexicoSt Petersburg State Tech Univ, St Petersburg 195251, RussiaTampere Univ Technol, Inst Mat Chem, FIN-33101 Tampere, FinlandBarmenkov, YO, Ctr Invest Opt, Loma Bosque 115, Leon 37150, Gto, Mexico
TI - Phase-modulated beams technique for thin photorefractive films characterization
AB - The phase-modulated beams technique is developed for nonlinear thin photorefractive films characterization. In the Raman-Nath diffraction approximation, the formulas are deduced, allowing us to measure the amplitude of phase grating recorded in a film and its nonlinear refractive index n(2). The method is applied for studying Langmuir-Blodgett multilayer thin (similar to 0.6 mu m) films of Bacteriorhodopsin at wavelength 633 nm. (C) 2000 American Institute of Physics. [S0003-6951(00)02514-6]
MH - Finland
MH - Mexico|Guanajuato
MH - Russia
PB - MELVILLE: AMER INST PHYSICS
RP - NOT IN FILE
U3 - TC 3
U4 - Physics, Applied
U5 - J;Article
AV - English
IS - 0003-6951
UR - ISI:000086134700003
L2 - BACTERIORHODOPSIN FILM
SO - Applied Physics Letters 2000 ;76(14):1801-1803
164
UI - 16401
AU - Barmenkov YO
AU - Kozhevnikov NM
AD - Ctr Invest & Opt, Leon, MexicoSt Petersburg State Tech Univ, St Petersburg, RussiaBarmenkov, YO, Ctr Invest & Opt, Leon, Mexico
TI - Kinetics of the distortions of dynamic gratings upon two-wave mixing in photorefractive media
AB - The results of computer simulation of the recording of dynamic phase gratings in reversible photosensitive media with strong local and nonlocal responses are presented. The self-diffraction of intense light beams recording a spatially displaced phase grating is shown to lead to a decrease in the effective thickness of the grating, inversion of its extrema, and the consequent formation of a central dip on the angular dependence of the diffraction efficiency. Formation of a phase grating by beams of unequal intensity in media with a local response is accompanied by discontinuous dynamics of the distortions of the fringes in the interference pattern and the phase grating, which lead to complicated irregular energy transfer between the beams in the initial stage of the recording process. (C) 2000 The Optical Society of America. [S1070-9762(00)01202-1]
MH - Mexico|Guanajuato
MH - Russia
PB - WASHINGTON: OPTICAL SOC AMER
RP - NOT IN FILE
U3 - TC 1
U4 - Optics
U5 - J;Article
AV - English
IS - 1070-9762
UR - ISI:000085767600012
L2 - CRYSTALS; DIFFRACTION; HOLOGRAMS
SO - Journal of Optical Technology 2000 ;67(2):145-148
165
UI - 16433
AU - Barmenkov YO
AU - Kir'yanov AV
AU - Starodumov AN
AU - Leppanen VP
AU - Vanhanen J
AU - Jaaskelainen T
AU - Kozhevnikov NM
AD - Ctr Invest Opt, Leon 37150, Guanajuato, MexicoUniv Joensuu, FIN-80101 Joensuu, FinlandSt Petersburg State Tech Univ, St Petersburg 195251, RussiaBarmenkov, YO, Ctr Invest Opt, Leon 37150, Guanajuato, Mexico
TI - Advanced model for a 4-keto Bacteriorhodopsin photocycle based on phase grating recording analysis
AB - Peculiarities of the phase grating recording in polymer films containing 4-keto Bacteriorhodopsin are investigated under absorption saturation. The phase-modulated beams technique is used to measure photoresponse from the films in real time. Three maxima of the photoresponse are detected. The first two (at similar to 1 and similar to 10 s) correspond to the positive amplitude of the phase grating, whereas the third maximum corresponds to the negative one (at similar to 1 min). This phenomenon is explained, as theoretical analysis shows, by the spatial distortions of the grating, resulting in the fundamental spatial harmonic sign exchange. These maxima, we believe, correspond to three photocycles in the 4-keto Bacteriorhodopsin molecule, for which a novel scheme is suggested. The results of theoretical simulations are shown to be in good agreement with the experiment
MH - Finland
MH - Mexico|Guanajuato
MH - Russia
PB - BIRMINGHAM: INTERPERIODICA
RP - NOT IN FILE
U3 - TC 2
U4 - Optics;Physics, Applied
U5 - J;Article
AV - English
IS - 1054-660X
UR - ISI:000085681600013
L2 - FILMS; ABSORPTION; HOLOGRAPHY
SO - Laser Physics 2000 ;10(1):60-63
166
UI - 15783
AU - Barnetche JM
AU - Flavell RA
AU - Madrid-Marina V
AU - Moreno J
AD - IMSS, Autoimmune Dis Res Unit, Mexico City, DF, MexicoYale Univ, Sch Med, New Haven, CT, USAInst Publ Hlth, Cuernavaca, Morelos, Mexico
TI - Deletion of early B cell precursors by constituive expresion of CD154 on B cells in transgenic mice
MH - Mexico|Distrito Federal
MH - Mexico|Morelos
MH - USA
PB - BETHESDA: FEDERATION AMER SOC EXP BIOL
RP - NOT IN FILE
U3 - TC 0
U4 - Biochemistry & Molecular Biology;Biology;Cell Biology
U5 - J;Meeting Abstract
AV - English
IS - 0892-6638
UR - ISI:000086643101621
SO - Faseb Journal 2000 ;14(6):A1187-A1187
167
UI - 14984
AU - Baron C
AU - Equihua LO
AU - Mestre JP
AD - Degremont SA, F-92508 Rueil Malmaison, FranceDegremont Mexico SA CV, Mexico City 11300, DF, MexicoBaron, C, Degremont SA, 183 Ave 18 Juin 1940, F-92508 Rueil Malmaison, France
TI - BOO Case: water management project for the use of reclaimed wastewater and desalted seawater for the "Antonio Dovali Jaime" refinery, Salina Cruz, Oaxaca, Mexico
AB - The water management project for the "Antonio Dovali Jaime" Refinery is definitely one of the firsts of its type that has been implemented in Mexico. The aim of this project is to reduce the water consumption through seawater desalination for steam generation and reclamation of treated wastewater for cooling purposes. For this purpose Pemex-Refinacion opened a bidding process under a Build-Own-and-Operate scheme. In 1995 the partnership formed by BICONSA, Degremont and Marubeni was awarded this project. The processes selected include: reverse osmosis for seawater desalination as well as biological treatment with nitrification-denitrification and tertiary treatment for industrial wastewater treatment. The constrution of this facility started at the end of 1997 and started its operation at the end of 1999
MH - France
MH - Mexico|Distrito Federal
PB - LONDON: I W A PUBLISHING
RP - NOT IN FILE
U3 - TC 0
U4 - Engineering, Environmental;Environmental Sciences;Water Resources
U5 - J;Review
AV - English
IS - 0273-1223
UR - ISI:000089995400006
L2 - wastewater reclamation;wastewater reuse;seawater desalination;refinery wastewater;BOO facility
SO - Water Science and Technology 2000 ;42(5-6):29-36
168
UI - 14885
AU - Barot M
AU - Brustle T
AU - de la Pena JA
AD - Univ Nacl Autonoma Mexico, Inst Matemat, Mexico City 04510, DF, MexicoUniv Bielefeld, Fak Math, D-4800 Bielefeld, GermanyBarot, M, Univ Nacl Autonoma Mexico, Inst Matemat, Ciudad Univ, Mexico City 04510, DF, Mexico
TI - Derived-tame tree algebras of type E
AB - Let A be an algebra whose quiver is a tree and denote by chi (A) the quadratic Euler form associated with A. Suppose A contains a convex subcategory which is derived equivalent to a hereditary algebra of type E-p (E) over bar (p)(p = 6, 7, 8) or to a tubular algebra. Then we show that the repetitive category of A is tame precisely when chi (A) is non-negative
MH - Germany
MH - Mexico|Distrito Federal
PB - BERLIN: WALTER DE GRUYTER & CO
RP - NOT IN FILE
U3 - TC 3
U4 - Mathematics, Applied;Mathematics
U5 - J;Article
AV - English
IS - 0933-7741
UR - ISI:000165364800004
SO - Forum Mathematicum 2000 ;12(6):713-721
169
UI - 16323
AU - Barraza GA
AU - Back WE
AU - Mata F
AD - Tecnol Monterrey, Dept Ind Engn, Monterrey 64849, NL, MexicoClemson Univ, Dept Civil Engn, Clemson, SC 29630, USATecnol Monterrey, Mgmt Grad Sch, Monterrey 64849, NL, MexicoBarraza, GA, Tecnol Monterrey, Dept Ind Engn, Monterrey 64849, NL, Mexico
TI - Probabilistic monitoring of project performance using SS-curves
AB - The purpose of this study was to develop a new concept of project control. This new concept uses stochastic S-curves (SS-Curves) as an alternative to using the deterministic S-curve technique commonly employed in professional practice. SS-curves are developed by determining the activity level variability in cost and duration. Simulation is the recommended approach for obtaining SS-curves, similar to the way chat stochastic schedules are currently developed. SS-curves provide probability distributions for expected, cost and duration for a given percentage of work completed. Monitoring project performance is performed by comparing the most: likely budget and duration values, obtained from respective probability distributions For actual progress, with the project's actual data and cumulative cost. By using this method, an evaluation of actual project performance can be developed that appropriately considers the natural variability of construction costs and duration, rather than utilizing only one possible deterministic outcome. Given the probabilistic characteristics of SS-curves, additional benefits are presented that enable a more comprehensive project control methodology
MH - Mexico|Nuevo Leon
MH - USA
PB - NEW YORK: ASCE-AMER SOC CIVIL ENGINEERS
RP - NOT IN FILE
U3 - TC 7
U4 - Construction & Building Technology;Engineering, Industrial;Engineering, Civil
U5 - J;Article
AV - English
IS - 0733-9364
UR - ISI:000086105800009
SO - Journal of Construction Engineering and Management-Asce 2000 ;126(2):142-148
170
UI - 16410
AU - Barrera JL
AU - Verastegui E
AU - Meneses A
AU - Zinser J
AU - de la Garza J
AU - Hadden JW
AD - Natl Inst Cancerol, Dept Surg, Mexico City, DF, MexicoNatl Inst Cancerol, Dept Med, Mexico City, DF, MexicoNatl Inst Cancerol, Dept Pathol, Mexico City, DF, MexicoUniv S Florida, Coll Med, Dept Internal Med, Div Immunopharmacol, Tampa, FL 33612, USAHadden, JW, 428 Harbor Rd, Cold Spring Harbor, NY 11724, USA
TI - Combination immunotherapy of squamous cell carcinoma of the head and neck - A phase 2 trial
AB - Objectives: To test the efficacy of a natural cytokine mixture (IRX-2), cyclophosphamide, indomethacin, and zinc to-induce immune regression of squamous cell carcinoma (SCC) of the head and neck (H&N) prior to conventional therapy and to characterize the responses. Patients and Design: A phase 2 trial was performed in 15 adults with recently diagnosed, biopsy-confirmed H&N SCC (3 with stage II disease, 6 with stage III disease, and 6 with stage IV disease). The patients were treated with 20 days of perilymphatic injections of IRX-2 (administered subcutaneously at the base of the skull) in combination with contrasuppression consisting of a low-dose infusion of cyclophosphamide (300 mg/m(2)), and daily oral indomethacin and zinc (StressTabs) in a 21-day cycle before surgery and/or radiotherapy. Tumor dimensions, toxic effects, and disease-free survival were monitored. The tumor sections were histologically examined after surgery, and tumor reduction, fragmentation, and lymphoid infiltration were assessed. Results: All 15 patients responded clinically to the 21-day IRX-2 protocol: 1 with a complete response, 7 with a partial response, and 7 with a minor response. All 15 patients responded pathologically with tumor reduction (mean, 42%) and fragmentation (mean, 50%) in the histological section and increased lymphoid infiltration. The adverse effects of the IRX-2 protocol were negligible except for an allergic skin rash (n = 1) and parotiditis (n = 1). Indomethacin caused gastritis in 1 patient. Reduction of pain and ulceration and bleeding were observed in 8 and 4 patients, respectively. Four of 5 patients with lymphopenia showed increased CD3, CD4, and CD8 cell counts. After surgery (n = 13) and/or radiotherapy (n = 10) and with a mean follow-up of 17 months, 3 patients have had recurrences, 1 patient has died of disease, 1 patient has been re-treated with immunotherapy and has no evidence of disease, and 1 patient is alive with disease. Two patients died of other causes with no evidence of disease. Conclusions: The IRX-2 immunotherapy induced lymphocyte mobilization and infiltration in H&N SCC associated with clinical and histological tumor responses indicative of immune regression in all 15 patients. Minimal toxic effects were observed, and overall survival may have been improved. A phase 3 trial seems warranted
MH - Mexico|Distrito Federal
MH - USA
PB - CHICAGO: AMER MEDICAL ASSOC
RP - NOT IN FILE
U3 - TC 17
U4 - Otorhinolaryngology;Surgery
U5 - J;Article
AV - English
IS - 0886-4470
UR - ISI:000085808500014
L2 - RECOMBINANT INTERLEUKIN-2; TUMOR-ANTIGENS; CANCER; CHEMOTHERAPY; REGRESSION; INJECTIONS
SO - Archives of Otolaryngology-Head & Neck Surgery 2000 ;126(3):345-351
171
UI - 16524
AU - Barrera RG
AU - Mendoza CI
AU - Fuchs R
AD - Univ Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoIowa State Univ, Ames Lab, Ames, IA 50011, USAIowa State Univ, Dept Phys & Astron, Ames, IA 50011, USABarrera, RG, Univ Nacl Autonoma Mexico, Inst Fis, Apartado Postal 20364, Mexico City 01000, DF, Mexico
TI - Electron energy-loss spectroscopy in systems of polarizable spheres
AB - We start with a brief presentation of the dielectric formalism used to calculate the energy loss of high-energy electrons (100 keV) passing through a random system of polarizable spheres embedded in a homogeneous matrix. The formalism is then extended to the case of electrons traveling parallel to a homogeneous slab of finite thickness in which either ordered or disordered collections of polarizable spheres are embedded. For an ordered system in which the spheres are in a cubic array, the calculated energy-loss spectra are compared with those of an alternative theory. For a slab with disordered collections of spheres we find the energy-loss spectra using the recursive Green's function method and compare our results with the available experimental data as well as with an extension of the semiclassical-infinite-barrier (SCIB) model. Finally, we discuss the relevance of our work as well as trends for future research. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Distrito Federal
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 0
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0921-4526
UR - ISI:000085314700009
L2 - electron energy-loss spectroscopy;spectral representation;recursive Green's function method;spherical inclusions;surface response function;LOSS SPECTRA; COMPOSITE; MEDIA
SO - Physica B 2000 ;279(1-3):29-32
172
UI - 15838
AU - Barrios VAE
AU - Najera RH
AU - Petit A
AU - Pla F
AD - Natl Autonomous Univ Mexico, Fac Quim, Dept Polimeros, Mexico City 04510, DF, MexicoEcole Natl Super Ind Chim, Inst Natl Polytech Lorraine, CNRS UMR 7568, Lab Chim Phys Macromol, F-54001 Nancy, FranceEcole Natl Super Ind Chim, Inst Natl Polytech Lorraine, CNRS UPR 6811, Lab Sci Genie Chim, F-54001 Nancy, FranceBarrios, VAE, Natl Autonomous Univ Mexico, Fac Quim, Dept Polimeros, Mexico City 04510, DF, Mexico
TI - Selective hydrogenation of butadiene-styrene copolymers using a Ziegler-Natta type catalyst 1. Kinetic study
AB - The hydrogenation of styrene-butadiene copolymers of known global composition, monomeric distribution, molecular weight and microstructure is here reported. The saturation was carried out through a sequential polymerization-hydrogenation process which efficiency relies on the use of the polymerization solvent and initiator (cyclohexane and n-butyllithium) as the hydrogenation solvent and catalyst promoter, respectively. The SBRs, dissolved in cyclohexane, were homogeneously hydrogenated using a Ziegler-Natta type catalyst, prepared with nickel acetylacetonate and n-butyllithium. The only species, which was not present in both parts of the global process, is the catalyst for the homogeneous hydrogenation: nickel acetylacetonate. Three types of SBRs were investigated on the basis of their monomeric distribution: diblock (D-SBR), triblock with polystyrene extremes (T-SBR) and random (R-SBR). All the copolymers studied were synthesized by anionic solution polymerization, The precursors and corresponding hydrogenated polymers were analyzed by infrared spectroscopy (FTIR) and nuclear magnetic resonance ((HNMR)-H-1) to determine the 1,2-vinyl and 1,4-trans double bond content in the butadiene portion of the copolymers. These data were used to calculate the saturation degree, X, considering the amount of double bonds of the precursor copolymers and the corresponding hydrogenated copolymer: X = (C-i0 - C-i)/C-i0. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - France
MH - Mexico|Distrito Federal
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 4
U4 - Polymer Science
U5 - J;Article
AV - English
IS - 0014-3057
UR - ISI:000087742500007
L2 - anionic block and random SBRs;homogeneous hydrogenation;Ziegler-Natta type catalyst;hydrogenation kinetics;POLYMERS; RUBBER
SO - European Polymer Journal 2000 ;36(9):1817-1834
173
UI - 15376
AU - Barthel R
AU - Piedrahita JA
AU - McMurray DN
AU - Payeur J
AU - Baca D
AU - Guemes FS
AU - Perumaalla VS
AU - Ficht TA
AU - Templeton JW
AU - Adams LG
AD - Texas A&M Univ, Coll Vet Med, Dept Vet Pathobiol, College Stn, TX 77843, USATexas A&M Univ, Coll Vet Med, Dept Vet Anat & Publ Hlth, College Stn, TX 77843, USATexas A&M Univ, Coll Med, Dept Med Microbiol & Immunol, College Stn, TX 77843, USANatl Vet Serv Labs, Ames, IA 50011, USATexas Anim Hlth Commiss, Austin, TX 78758, USAUniv Nacl Autonoma Mexico, Fac Med Vet & Zootecnia, Dept Microbiol & Inmunol, Mexico City 04510, DF, MexicoBarthel, R, Texas A&M Univ, Coll Vet Med, Dept Vet Pathobiol, College Stn, TX 77843 USA
TI - Pathologic findings and association of Mycobacterium bovis infection with the bovine NRAMP1 gene in cattle from herds with naturally occurring tuberculosis
AB - Objective-To determine necropsy and Mycobacterium bovis culture results in cattle from herds with tuberculosis, the role of the bovine NRAMP1 gene rn resistance and susceptibility to infection with M bovis, and the association between magnitude of the tuberculous lesions and various types of M bovis isolates. Animals-61 cattle from herds with tuberculosis in Texas and Mexico. Procedure-61 cattle were evaluated by necropsy; 59 had positive and 2 had negative caudal fold tuberculin intradermal lest (CFT) results. Thirty-three cattle with positive CFT results were genotyped to evaluate polymorphism of the 3' untranslated region of the bovine NRAMP1 gene, using single-stranded conformational analysis, 9 were resistant to M bovis with no tuberculous lesions and negative M bovis culture results, and 24 were susceptible with tuberculous lesions and positive M bovis culture results. Isolates of M bovis were analyzed by restriction fragment length polymorphism (RFLP) on the basis of IS6110 sequences and direct-repeat fingerprinting patterns. Results-21 (35.6%; 21/59) cattle with positive CFT results had tuberculous lesions or positive culture results; in addition, 1 of 2 cattle with negative CFT results had tuberculous lesions and positive culture results. Tuberculous lesions were most common in the thorax (35/63, 55.5%) and lymphoid tissues of the head (10/63; 15.9%). Tuberculous lesions varied from 1 to 11/animal; 8 of 21 (38.1%) had solitary lesions. Associations were not found between resistance or susceptibility to infection with M bovis and polymorphism in the NRAMP1 gene or between the magnitude of the lesions and various RFLP types of M bovis isolates. Conclusions and Clinical Relevance-The NRAMP1 gene does not determine resistance and susceptibility to infection with M bovis in cattle
MH - Mexico|Distrito Federal
MH - USA
PB - SCHAUMBURG: AMER VETERINARY MEDICAL ASSOC
RP - NOT IN FILE
U3 - TC 17
U4 - Veterinary Sciences
U5 - J;Article
AV - English
IS - 0002-9645
UR - ISI:000089078400024
L2 - RESISTANCE; SUSCEPTIBILITY; MICE; BCG; LESIONS; STRAINS
SO - American Journal of Veterinary Research 2000 ;61(9):1140-1144
174
UI - 14975
AU - Bartnicki-Garcia S
AU - Bracker CE
AU - Gierz G
AU - Lopez-Franco R
AU - Lu HS
AD - Univ Calif Riverside, Dept Plant Pathol, Riverside, CA 92521, USAUniv Calif Riverside, Dept Math, Riverside, CA 92521, USAPurdue Univ, Dept Bot & Plant Pathol, W Lafayette, IN 47907, USAInst Tecnol & Estudios Super, Ctr Biotecnol, Monterrey 64849, MexicoBartnicki-Garcia, S, Univ Calif Riverside, Dept Plant Pathol, Riverside, CA 92521 USA
TI - Mapping the growth of fungal hyphae: Orthogonal cell wall expansion during tip growth and the role of turgor
AB - By computer-enhanced videomicroscopy, we mapped the trajectory of external and internal cell surface markers in growing fungal hyphae to determine the pattern of cell wall expansion during apical growth, Carbon particles (India ink) were chosen as external markers for tip expansion of Rhizoctonia solani hyphae. Irregularities in the growing apical walls of R. solani sewed as internal markers. Marker movement was traced in captured frames from the videotaped sequences. External and internal markers both followed orthogonal trajectories; i.e., they moved perpendicular to the cell surface regardless of their initial position in the hyphal apex. We found no evidence that the tip rotates during elongation. The discovery that the cell wall of a growing hypha expands orthogonally has major repercussions on two fronts: 1) It supports the long-held view that turgor pressure is the main force driving cell wall expansion. 2) It provides crucial information to complete the mathematical derivation of a three-dimensional model of hyphal morphogenesis based on the vesicle supply center concept. In three dimensions, the vesicle gradient generated by the vesicle supply center is insufficient to explain shape; it is also necessary to know the manner in which the existing surface is displaced during wall expansion
MH - USA
MH - Mexico|Nuevo Leon
PB - BETHESDA: BIOPHYSICAL SOCIETY
RP - NOT IN FILE
U3 - TC 21
U4 - Biophysics
U5 - J;Article
AV - English
IS - 0006-3495
UR - ISI:000165104500015
L2 - CANDIDA-ALBICANS; COMPUTER-SIMULATION; MORPHOGENESIS; SPITZENKORPER; DETERMINES; BEHAVIOR
SO - Biophysical Journal 2000 ;79(5):2382-2390
175
UI - 16167
AU - Bartolo-Perez P
AU - Pena JL
AU - Salas FH
AU - Wheat HG
AU - Hernandez-Duque G
AD - IPN, CINVESTAV, Unidad Merida, Merida 97310, Yuc, VenezuelaUniv Oviedo, Dept Fis, E-33007 Oviedo, SpainUniv Texas, Dept Mech Engn, Austin, TX 78712, USAUniv Mayab, Fac Ingn, Merida 97310, Yuc, MexicoBartolo-Perez, P, IPN, CINVESTAV, Unidad Merida, AP 73 Cordemex, Merida 97310, Yuc, Venezuela
TI - Corrosion of reinforced steel bars embedded in concrete: A study of electrochemical and surface analysis
AB - We present a study of corrosion of reinforced steel bars embedded in concrete, We carried out both electrochemical analysis /E-corr polarization resistance (R-p), and electrochemical impedance spectroscopy (EIS)I and surface analysis by AES, XPS, SEM, and EDAX. We found that 1/R-p >28 mu S/cm(2), which gives I-corr > 0.73 mu A/cm(2), indicating that severe corrosion was occurring. After a 20-week exposure, the Nyquist plot of the electrochemical impedance Z(j omega) showed two capacitive arcs and rests of a third one, the corresponding time constants RC being related to the double layer, the interfacial thin film, and the concrete matrix, respectively. The interfacial thin film resistance (R-f) and the double-layer resistance (R-ct) are found to be about 220 Omega and 320 Omega, respectively. Departure from the capacitive semi-circles is observed, indicating the presence of diffusion-driven corrosion. Analysis of AES allowed us to determine the concentration of corrosion products on the surface and in the near surface region. Migration of S, C, and Ca to the surface was observed. From the XPS spectra we conclude, at room temperature, the existence of the following iron compounds: Fe2O3, and FeCl2, as well as the formation of CaCO3; these compounds appear before an inner iron-chromium oxide. SEM and EDAX show am existance of inhomogeneous corrosion in the inner layers
MH - Mexico|Yucatan
MH - Spain
MH - USA
MH - Venezuela
PB - LONDON: FREUND PUBLISHING HOUSE LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Electrochemistry;Metallurgy & Metallurgical Engineering;Materials Science, Coatings & Films
U5 - J;Article
AV - English
IS - 0048-7538
UR - ISI:000086524000009
L2 - corrosion;reinforced steel;electrochemical impedance;surface analysis
SO - Corrosion Reviews 2000 ;18(2-3):255-266
176
UI - 11414
AU - Baruch IS
AU - Flores JM
AU - Martinez JC
AU - Nenkova B
AD - IPN, CINVESTAV, Mexico City 07360, DF, MexicoBAS, IIT, Sofia, BulgariaNenkova, B, IPN, CINVESTAV, Av IPN 2508,AP 14470, Mexico City 07360, DF, Mexico
TI - Fuzzy-neural models for real-time identification and control of a mechanical system
AB - A two-layer Recurrent Neural Network Model (RNNM) and an improved Backpropagation-through-time method of its learning are described. For a complex nonlinear plants identification, a fuzzy-neural multi-model, is proposed. The proposed fuzzy-neural model, containing two RNNMs is applied for real-time identification of nonlinear mechanical system. The simulation and experimental results confirm the RNNM applicability
MH - Bulgaria
MH - Mexico|Distrito Federal
PB - BERLIN: SPRINGER-VERLAG BERLIN
RP - NOT IN FILE
U3 - TC 0
U4 - Computer Science, Artificial Intelligence
U5 - S;Article
AV - English
IS - 0302-9743
UR - ISI:000174951600028
L2 - FRICTION COMPENSATION; DC MOTOR; HYSTERESIS
SO - Artificial Intelligence: Methodology, Systems, Applications, Proceedings 2000 ;1904():292-300
177
UI - 16022
AU - Bashan Y
AU - Davis EA
AU - Carrillo-Garcia A
AU - Linderman RG
AD - USDA ARS, Hort Crops Res Lab, Corvallis, OR 97330, USACIB, Ctr Biol Res NW, La Paz 23000, MexicoLinderman, RG, USDA ARS, Hort Crops Res Lab, 3420 NW Orchard Ave, Corvallis, OR 97330 USA
TI - Assessment of VA mycorrhizal inoculum potential in relation to the establishment of cactus seedlings under mesquite nurse-trees in the Sonoran Desert
AB - A commonly observed preferential association was quantified between mature native mesquite (Prosopis articulata) trees and the seedlings of six cactus species (Pachycereus pringlei, Opuntia cholla, Lophocereus schottii, Machaerocereus gummosus, Lemaireocereus thurberi, Mammilaria sp.) in a previously-disturbed area of the Sonoran Desert of Baja California, Mexico. We hypothesized that, in addition to more favorable edaphic factors, the inoculum potential of beneficial vesicular-arbuscular mycorrhizal (VAM) fungi was higher, and therefore, more favorable for cactus seedling establishment under the mesquite tree canopy (UC) compared to adjacent barren areas (BAs) away from the trees. In the greenhouse inoculum potential assays, VAM fungi were detected in onion (Allium cepa) trap plants from all soil samples regardless of collection site, but cardon cactus (P. pringlei) trap seedlings formed no VAM even after 6.5 months. Test soils were further used to preinoculate new onion seedlings transplanted into pots, to serve as nurse plants to inoculate adjacent cardon seedlings by vegetative transfer. After 15 months, cardon seedlings did develop slight VAM colonization, confined exclusively to the outermost cortical layers. Examination of test soils for spores or root fragments revealed very few to none, and spore production on onion trap plant roots was also sparse even though colonization was high. Analysis of UC and BA soils revealed that the water holding capacity, nutrient content, cation exchange capacity, total carbon, and total nitrogen contents of the UC soils were all higher than those of the BA soils. Since the VAM inoculum density in this study was not different between sites under and away from the mesquite tree canopy, we concluded that VAM inoculum density is not the primary factor for the establishment of cactus seedlings and that edaphic factors probably play a more important role. Our results suggest, however, that VAM inoculum potential in these hot desert soils, although relatively low, is probably maintained in the upper layers by means of hyphal fragments rather than spores. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Baja California Sur
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 17
U4 - Soil Science
U5 - J;Article
AV - English
IS - 0929-1393
UR - ISI:000087104200008
L2 - desert revegetation;inoculum potential;soil disturbance;Sonoran desert;vesicular-arbuscular mycorrhizae;VAM fungi;BAJA-CALIFORNIA; FUNGI; PLANTS; GROWTH; SOIL; MEXICO
SO - Applied Soil Ecology 2000 ;14(2):165-175
178
UI - 15040
AU - Bashir A
AU - Kizilersu A
AU - Pennington MR
AD - Univ Michoacana San Nicolas de Hidalgo, Inst Fis & Matemat, Morelia, Michoacan, MexicoUniv Adelaide, Special Res Ctr Subatom Struct Matter, Adelaide, SA 5005, AustraliaUniv Adelaide, Dept Phys & Math Phys, Adelaide, SA 5005, AustraliaUniv Durham, Ctr Particle Theory, Durham DH1 3LE, EnglandBashir, A, Univ Michoacana San Nicolas de Hidalgo, Inst Fis & Matemat, Apdo Postal 2-82, Morelia, Michoacan, Mexico
TI - Does the weak coupling limit of the Burden-Tjiang deconstruction of the massless quenched three-dimensional QED vertex agree with perturbation theory?
AB - We derive constraints on the non-perturbative 3-point fermion-boson transverse vertex in massless QED3 from its perturbative calculation to order alpha. We also check the transversality condition to two loops and evaluate the fermion propagator to the same order. We compare a conjecture of the non-perturbative vertex by Burden and Tjiang against our results and comment on its drawbacks. Our calculation calls for the need to construct a non-perturbative form for the fermion-boson vertex which agrees with its perturbative limit to O(alpha)
MH - Australia
MH - United Kingdom
MH - Mexico|Michoacan
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 8
U4 - Astronomy & Astrophysics;Physics, Particles & Fields
U5 - J;Article
AV - English
IS - 0556-2821
UR - ISI:000089977200068
L2 - QUANTUM ELECTRODYNAMICS; 3-POINT VERTEX; GAUGE
SO - Physical Review D 2000 ;6208(8):
179
UI - 16026
AU - Basiuk VA
AU - Van Meervelt L
AU - Soloshonok VA
AU - Basiuk EV
AD - Univ Nacl Autonoma Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoUniv Arizona, Dept Chem, Tucson, AZ 85721, USAKatholieke Univ Leuven, Dept Chem, B-3001 Heverlee, BelgiumUniv Nacl Autonoma Mexico, Inst Quim, Mexico City 04510, DF, MexicoBasiuk, VA, Univ Nacl Autonoma Mexico, Inst Ciencias Nucl, Circuito Exterior CU,A Postal 70-543, Mexico City 04510, DF, Mexico
TI - 2,2,5,5,8,8-Hexamethyl-2,3,5,6,7,8-hexahydroimidazo[1,2-a]pyrazine-3,6-d ione, a bicyclic product of alpha-aminoisobutyric acid condensation
AB - The title compound, C12H19N3O2, is an unusual product of silica-catalyzed intermolecular condensation of alpha-amino-isobutyric acid. The molecule has three types of C-N bonds: a double bond, a cis-amide bond and single bonds, two of which are typical and two having intermediate lengths due to pi-electron delocalization between C=N and C=O groups. The cis-amide moieties interact to form dimers via hydrogen bonds which stack in parallel layers
MH - Belgium
MH - Mexico|Distrito Federal
MH - USA
PB - COPENHAGEN: MUNKSGAARD INT PUBL LTD
RP - NOT IN FILE
U3 - TC 6
U4 - Crystallography
U5 - J;Article
AV - English
IS - 0108-2701
UR - ISI:000087105800037
L2 - SPECTROSCOPY MASS-SPECTROMETRY; IDENTIFICATION; PYROLYSIS
SO - Acta Crystallographica Section C-Crystal Structure Communications 2000 ;56():598-599
180
UI - 16065
AU - Basiuk VA
AU - Navarro-Gonzalez R
AU - Benilan Y
AU - Raulin F
AD - Natl Autonomous Univ Mexico, Inst Ciencias Nucl, Lab Quim Plasmas & Estudios Planetarios, Mexico City 04510, DF, MexicoUniv Paris 12, UMR CNRS 7583, Lab Interuniv Syst Atmospher, F-94010 Creteil, FranceUniv Paris 07, UMR CNRS 7583, Lab Interuniv Syst Atmospher, F-94010 Creteil, FranceBasiuk, VA, Natl Autonomous Univ Mexico, Inst Ciencias Nucl, Lab Quim Plasmas & Estudios Planetarios, Circuito Exterior CU,A Postal 70-543, Mexico City 04510, DF, Mexico
TI - PM3, AM1, MINDO3 semi-empirical IR spectra simulations for some nitriles of interest for Titan's chemistry
AB - A set of the semi-empirical methods (PM3. AM1, MNDO and MINDO3) has been tested to find the best auxiliary tool for the identification of nitriles by gas chromatography/Fourier transform IR spectroscopy/mass spectrometry, considering five nitriles of interest for Titan's chemistry as test compounds: acetonitrile, acrylonitrile, cyanoacetylene, 2-butynenitrile and dicyanoacetylene. Of the four semi-empirical methods, MNDO can be considered as the most advantageous auxiliary tool for the gas chromatography/Fourier transform IR spectroscopy/mass spectrometry (GC/FTIR/MS) identification of nitriles of interest for Titan's atmospheric chemistry, since (1) the simulated IR spectra best match the experimental (in some cases AMI gives comparable results); (2) it provides the best linearity between the calculated and experimental frequencies (correlation coefficient of 0.990); a scaling factor of 0.90 Can be applied to afford better correspondence between the calculated and experimental wavenumbers. At the same time, none of the methods is able to predict infrared intensities and a spectral intensity pattern. (C) 2000 Elsevier Science B.V. All rights reserved
MH - France
MH - Mexico|Distrito Federal
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 7
U4 - Spectroscopy
U5 - J;Article
AV - English
IS - 1386-1425
UR - ISI:000086822500013
L2 - SPECTROSCOPY MASS-SPECTROMETRY; INFRARED-SPECTRA; BAND INTENSITY; AMINO-ACIDS; IDENTIFICATION; PRODUCTS; ATMOSPHERE; CONDENSATION; PYROLYSIS; AEROSOLS
SO - Spectrochimica Acta Part A-Molecular and Biomolecular Spectroscopy 2000 ;56(6):1157-1165
181
UI - 14650
AU - Bassol S
AU - Alvarado A
AU - Celis C
AU - Cravioto MC
AU - Peralta O
AU - Montano R
AU - Novelli J
AU - Albornoz H
AU - Kesseru E
AU - Soares A
AU - Petracco A
AU - Isaia B
AU - Mendes J
AU - Bahamondes L
AU - de Melo NR
AU - Reyes-Marquez R
AU - Albrecht G
AD - Univ Autonoma Coahuila, Ctr Invest Biomed, Torreon 27000, Coahuila, MexicoInst Nacl Perinatol, Mexico City, DF, MexicoHosp Gineco Obstetr Luis Castelazo Ayala, Mexico City 11455, DF, MexicoInst Nacl Nutr Salvador Zubiran, Dept Reprod Biol, Mexico City 14000, DF, MexicoHosp Clin Sn Borja Arriaran, Santiago, ChileHosp Carlos van Buren, Valparaiso, ChileHosp Frances, Buenos Aires, DF, ArgentinaHosp Clin, Buenos Aires, DF, ArgentinaSanta Casa Misericordia Rio de Janeiro, Serv Ginecol, Rio De Janeiro, BrazilPontificia Univ Catolica Rio de Janeiro, Ctr Clin, BR-22453 Rio De Janeiro, BrazilSanta Casa Misericordia Sao Paolo, Sao Paulo, BrazilCtr Pesquisas & Controle Doencas Materno Infantis, Campinas, SP, BrazilUniv Sao Paulo, Hosp Clin, Sao Paulo, BrazilCanada Latinoamer SA CV, Ctr Estrategico, Mexico City, DF, MexicoBassol, S, Univ Autonoma Coahuila, Ctr Invest Biomed, Calle Gregorio A Garcia 198 Sur, Torreon 27000, Coahuila, Mexico
TI - Latin American experience with two low-dose oral contraceptives containing 30 mu g ethinylestradiol/75 mu g gestodene and 20 mu g ethinylestradiol/150 mu g desogestrel
AB - The objective of this study was to compare cycle control, efficacy and tolerance of an oral contraceptive containing 20 mug ethinylestradiol and 150 mug desogestrel with a preparation containing 30 mug ethinylestradiol combined with 75 mug gestodene. This study involved 342 women and 4104 cycles use in Argentina, Brazil, Chile, and Mexico. Contraceptive efficacy was good with both formulations. Two pregnancies occurred in the desogestrel group but were not due to method failure. With respect to cycle control, the incidence of intermenstrual bleeding was higher during the first 3 cycles in the desogestrel group; it was significant (p <0.01) during the first 3 days of the cycle for a normal or heavy bleeding only in the Mexican group. Amenorrhea was not reported for any group, but the incidence of dysmenorrhea was significantly higher (p <0.01) in the Brazilian desogestrel group (13.8%) and was significantly lower (p <0.01) in the Mexican gestodene group (8.5%). Adverse events were similar in all the countries with headache, breast tension, and nausea, the most frequently reported symptoms. The range of mean increase in body weight varied from 0.2 kg in the Argentine group to 2.6 kg in the Chilian group (95% confidence limit, +/- 2.51) in the gestodene group, and 0.2 kg in the Argentine group to 2.5 kg in Brazilian group (95% confidence limit, +/- 2.36) in the desogestrel group. Fifteen women discontinued because of headache, but there were no significant differences between the groups regarding discontinuation for this and other medical or non-medical reasons. Both oral contraceptive preparations are reliable and well tolerated, and both have favorable effects on control cycle. (C) 2000 Elsevier Science Inc. All rights reserved
MH - Argentina
MH - Brazil
MH - Chile
MH - Mexico|Coahuila
MH - Mexico|Distrito Federal
PB - NEW YORK: ELSEVIER SCIENCE INC
RP - NOT IN FILE
U3 - TC 4
U4 - Obstetrics & Gynecology
U5 - J;Article
AV - English
IS - 0010-7824
UR - ISI:000165953900005
L2 - ethinylestradiol;desogestrel;gestodene;intermenstrual bleeding;dysmenorrhea;CYCLE CONTROL
SO - Contraception 2000 ;62(3):131-135
182
UI - 15566
AU - Bassol S
AU - Cravioto MC
AU - Durand M
AU - Bailon R
AU - Carranza S
AU - Fugarolas J
AU - Gaona R
AU - Parada LM
AU - Celis C
AU - Santoyo S
AU - Garza-Flores J
AU - Vazquez L
AU - Lopez C
AU - Gurucharri C
AU - Novelli J
AU - de Oliveira HC
AU - Mendez J
AU - de Andrade ME
AU - de Mello NR
AU - de Melo K
AU - Chada E
AU - Yassle ME
AU - Castaneda A
AU - Gomez P
AU - Arboleda C
AU - Trujillo L
AU - Bucheli R
AU - Hidalgo I
AU - Olavide R
AU - Parejarios J
AU - Succar J
AU - Reyes-Marquez R
AU - Albrecht G
AD - Univ Autonoma Coahuila, Ctr Invest Biomed, Torreon 27000, Coahuila, MexicoCtr Asistencia Reprod Humana AC, Mexico City, DF, MexicoInst Modelo Ginecol & Obstet, Cordova, ArgentinaHosp Rivadavia, Buenos Aires, DF, ArgentinaHosp Frances, Buenos Aires, DF, ArgentinaHosp Univ Pedro Ernesto Estadual Rio de Janeiro, Rio De Janeiro, BrazilSanta Casa Misericordia Sao Paulo, Sao Paulo, BrazilCtr Reprod Humana & Fertilizacao Assistida, Curitiba, Parana, BrazilUniv Sao Paulo, Hosp Clin, Fac Med, Sao Paula, BrazilUniv Sao Paulo, Fac Med Ribeirao Preto, Hosp Clin, Sao Paula, BrazilProfamilia, Medellin, ColombiaInst Materno Infantil, Bogota, ColombiaClin Seguro Social, Cali, ColombiaHosp Gen Medellin, Medellin, ColombiaClin Privada Quito, Quito, EcuadorClin Privada Guayaquil, Guayaquil, EcuadorBassol, S, Univ Autonoma Coahuila, Ctr Invest Biomed, Calle Gregorio A Garcia 198 Sur, Torreon 27000, Coahuila, Mexico
TI - Mesigyna (R) once-a-month combined injectable contraceptive: Experience in Latin America
AB - A phase III clinical study was carried out among 534 fertile Latin American women to evaluate cycle control, side effects, and contraceptive efficacy of a once-a-month combined injectable, Mesigyna, consisting of 50 mg norethisterone enanthate and 5 mg estradiol valerate. The pregnancy rate at 1 year was 0 per 100 woman-years for a total experience of 4688 woman-months. The overall discontinuation rate at one year was 17.9%. Discontinuation rate for bleeding problems was 5.2%. The Colombian women had a significant increase (p <0.001) in bleeding problems compared to other countries. The discontinuation rate for amenorrhea was 1.1%. There were no significant differences between the groups regarding discontinuation for other medical or non-medical reasons. Mean weight gain after one year of use was 1.02 kg. Mesigyna is an appropriate once-a-month injectable contraceptive for Latin American women since it is highly effective and its perception of normal menstrual bleeding is of importance in the Latin American population. (C) 2000 Elsevier Science Inc. All rights reserved
MH - Argentina
MH - Brazil
MH - Colombia
MH - Ecuador
MH - Mexico|Coahuila
MH - Mexico|Distrito Federal
PB - NEW YORK: ELSEVIER SCIENCE INC
RP - NOT IN FILE
U3 - TC 3
U4 - Obstetrics & Gynecology
U5 - J;Article
AV - English
IS - 0010-7824
UR - ISI:000088442300003
L2 - Mesigyna;once-a-month injectable contraceptive;menstrual bleeding;COMPARATIVE CLINICAL-TRIAL; INTRAMUSCULAR INJECTION; BLEEDING PATTERNS; CHINESE WOMEN; CYCLOFEM; NO.1
SO - Contraception 2000 ;61(5):309-316
183
UI - 16288
AU - Bassy O
AU - Jimenez-Garcia LF
AU - Echeverria OM
AU - Vazquez-Nin GH
AU - de la Espina SMD
AD - CSIC, Ctr Invest Biol, Dpto Biol Vegetal, Lab Matriz Nucl, E-28006 Madrid, SpainUNAM, Fac Ciencias, Dpto Biol, Lab Microscopia Elect, Mexico City, DF, Mexicode la Espina, SMD, CSIC, Ctr Invest Biol, Dpto Biol Vegetal, Lab Matriz Nucl, Velazquez 144, E-28006 Madrid, Spain
TI - High resolution detection of rRNA and rDNA in plant nucleoli with different activities by in situ hybridization
AB - Ln the present work we perform in situ hybridization with probes to different stretches of rDNA and electron microscopy of nucleoli with different activities, to gain insight into the ultrastructural organization of transcription and processing in the plant nucleolus. The main ultrastructural nucleolar components: fibrillar centers (FC), dense fibrillar component (DFC), and granular component (GC), are arranged in different ways depending on nucleolar activity. Heterogeneous FCs containing RNP fibrils and nucleolar perichromatin granules are frequently seen in nucleoli in the process of activation. DNA-RNA in situ hybridization with biotinylated probes spanning different sequences of the rDNA unit followed by immunogold detection of biotin, demonstrated the localization of the ribosomal transcripts in DFC, mainly in the zones around the FCs, in GC, and in the periphery of pale FC. The internal region of the heterogeneous FCs is labeled only in cells in the process of activation of transcription after dormancy. The distribution of the U3 probe indicates that the processing of the rRNA takes place in the DFC and inside the heterogeneous FCs, in which transcription occurs. DNA-DNA hybridization demonstrates the presence of rDNA in the compact and extended chromatin located in the interior and at the periphery of I;Cs and in nucleolar associated chromatin. Our results support the view that the plant nucleolus has a highly dynamic morphological and functional organization composed of a bipartite domain formed by FCs surrounded by DFC, which is associated with rRNA transcription and processing, and the GC representing a store of preribosomal particles. 2000 (C) Editions scientifiques et medicales Elsevier SAS
MH - Mexico|Distrito Federal
MH - Spain
PB - PARIS CEDEX 15: EDITIONS SCIENTIFIQUES MEDICALES ELSEVIER
RP - NOT IN FILE
U3 - TC 12
U4 - Cell Biology
U5 - J;Article
AV - English
IS - 0248-4900
UR - ISI:000086178900005
L2 - plant cells;nucleolus;rRNA;rDNA;ultrastructure;RIBOSOMAL-RNA GENES; DIFFERENT PATTERNS; FIBRILLAR CENTERS; PISUM-SATIVUM; CELL-CYCLE; HELA-CELLS; TRANSCRIPTION; ORGANIZATION; ULTRASTRUCTURE; AUTORADIOGRAPHY
SO - Biology of the Cell 2000 ;92(1):59-70
184
UI - 14689
AU - Batista CVF
AU - Gomez-Lagunas F
AU - Lucas S
AU - Possani LD
AD - Natl Autonomous Univ Mexico, Inst Biotechnol, Dept Mol Recognit & Struct Biol, Cuernavaca 62210, Morelos, MexicoNatl Autonomous Univ Mexico, Sch Med, Dept Physiol, Mexico City 04510, DF, MexicoInst Butantan, Sao Paulo, BrazilPossani, LD, Natl Autonomous Univ Mexico, Inst Biotechnol, Dept Mol Recognit & Struct Biol, Ave Univ 2001,POB 510-3, Cuernavaca 62210, Morelos, Mexico
TI - Tcl, from Tityus cambridgei, is the first member of a new subfamily of scorpion toxin that blocks K+-channels
AB - A new peptide, Tc1, containing only 23 amino acids closely packed by three disulfide bridges was isolated from the Amazonian scorpion Tityus cambridgei. It blocks reversibly the Shaker B K+-channels with a K-d of 65 nM and displaces binding of noxiustoxin to mouse brain synaptosome membranes. It is the shortest known peptide from scorpion venom that recognizes K+-channels and constitutes a new structural subfamily of toxin, classified as alphaKTx 13.1. (C) 2000 Federation of European Biochemical Societies. Published by Elsevier Science B.V. All rights reserved
MH - Brazil
MH - Mexico|Distrito Federal
MH - Mexico|Morelos
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 25
U4 - Biochemistry & Molecular Biology;Biophysics;Cell Biology
U5 - J;Article
AV - English
IS - 0014-5793
UR - ISI:000165897100007
L2 - scorpion toxin;K+-channel;Tityus cambridgei;PANDINUS IMPERATOR; NOXIUSTOXIN; PEPTIDES; VENOM
SO - Febs Letters 2000 ;486(2):117-120
185
UI - 15179
AU - Baumgardner D
AU - Raga GB
AU - Kok G
AU - Ogren J
AU - Rosas I
AU - Baez A
AU - Novakov T
AD - Univ Nacl Autonoma Mexico, Ctr Ciencias Atmosfera, Mexico City 04510, DF, MexicoNatl Ctr Atmospher Res, Boulder, CO 80307, USAUniv Calif Berkeley, Berkeley Natl Lab, Berkeley, CA 94720, USANOAA, CMDL, Boulder, CO 80303, USABaumgardner, D, Univ Nacl Autonoma Mexico, Ctr Ciencias Atmosfera, Circuito Exteriro,Ciudad Univ, Mexico City 04510, DF, Mexico
TI - On the evolution of aerosol properties at a mountain site above Mexico City
AB - Size distributions, scattering and absorption coefficients, and the bulk chemical composition of aerosols have been measured at a mountain site 400 m above the southwest sector of the Mexico City basin during a two-week period in November 1997. Variations in these properties are primarily related to local meteorology, i.e., wind direction and relative humidity; however, a link was found between carbon monoxide and ozone and the partitioning of aerosols between Aitken and accumulation mode sizes. Relative humidity was also found to affect this partitioning of aerosol size and volume. In addition, the fraction of sulfate in the aerosols was much higher on a high-humidity day than on a very low humidity day; however, the fraction of the mass contained in organic and elemental carbon was the same regardless of humidity levels. The daily variations of aerosol properties are associated with the arrival of new particles at the research site transported from the city basin and their subsequent mixture with aged aerosols that remain in the residual layer from the night before
MH - Mexico|Distrito Federal
MH - USA
PB - WASHINGTON: AMER GEOPHYSICAL UNION
RP - NOT IN FILE
U3 - TC 22
U4 - Meteorology & Atmospheric Sciences
U5 - J;Article
AV - English
IS - 0747-7309
UR - ISI:000089469100010
L2 - AIR-POLLUTION; MORTALITY; PARTICLES
SO - Journal of Geophysical Research-Atmospheres 2000 ;105(D17):22243-22253
186
UI - 15328
AU - Bautista-Banos S
AU - Hernandez-Lopez M
AU - az-Perez JC
AU - Cano-Ochoa CF
AD - Ctr Desarrollo Prod Biot, Yautepec 62731, Morelos, MexicoInst Tecnol Zacatepec, Morelia, Michoacan, MexicoUniv Georgia, Dept Hort, Coastal Plain Expt Stn, Tifton, GA 31793, USABautista-Banos, S, Ctr Desarrollo Prod Biot, Carr Yautepec Jojutla Km 8-5, Yautepec 62731, Morelos, Mexico
TI - Evaluation of the fungicidal properties of plant extracts to reduce Rhizopus stolonifer of 'ciruela' fruit (Spondias purpurea L.) during storage
AB - Rhizopus stolonifer is one of the main postharvest pathogens of 'ciruela' fruit (red mombin) (Spondias purpurea L.) during handling and storage. To evaluate the fungicidal potential of plants indigenous to the state of Morelos, Mexico, aqueous extracts of leaves or stems of 19 different plant species were tested against Rhizopus development in vitro and in vivo. Extracts were applied to fruit of three botanical varieties of ciruela: fruit Skin turning green to Icd, green to yellow or green to orange, grown throughout the year over dry and wet seasons. In vitro evaluations were carried out to observe mycelial growth, sporulation and conidial germination. Evaluations on fruit were percentage and disease severity, soluble solids content (SSC) and weight loss after 4 days storage at ambient temperature. In general, leaf extracts had better fungicidal effects than stem extracts. For in vitro studies, leaf extracts inhibited sporulation and spore germination more than mycelial development. Leaf extracts of Annona cherimola, Bromelia hemisphaerica and Curica papaya inhibited Rhizopus sporulation and rot development on the yellow variety whereas extracts of Casimiroa edulis reduced R. stolonifer rot on red ciruela. Infection spread from 25 to 100% of the fruit surface depending on extract or ciruela variety. After storage, SSC values were not significantly different. Less weight loss was observed for the orange variety than the other varieties. Further studies need to be undertaken to isolate the active compounds from those extracts with fungicidal potential. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Michoacan
MH - Mexico|Morelos
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 3
U4 - Agronomy;Food Science & Technology;Horticulture
U5 - J;Article
AV - English
IS - 0925-5214
UR - ISI:000089047700010
L2 - red mombin;yellow mombin;biofungicides;postharvest rots;aqueous extracts;PAPAYA
SO - Postharvest Biology and Technology 2000 ;20(1):99-106
187
UI - 15469
AU - Bautista R
AU - Crawley-Boevey W
AU - Lei TG
AU - Zhang YB
AD - Univ Nacl Autonoma Mexico, Inst Math, Mexico City 04510, DF, MexicoUniv Leeds, Dept Pure Math, Leeds LS2 9JT, W Yorkshire, EnglandBeijing Normal Univ, Dept Math, Beijing 100875, Peoples R ChinaBautista, R, Univ Nacl Autonoma Mexico, Inst Math, Mexico City 04510, DF, Mexico
TI - On homogeneous exact categories
AB - In the present paper we prove that a certain subcategory E of the module category over some infinite-dimensional algebra R has almost split sequences and strongly homogeneous property; i.e., for each indecomposable module M in E, there is an almost split sequence starting and also ending at M. It is also proved that except for a trivial case, E is of wild representation type, (C) 2000 Academic Press
MH - United Kingdom
MH - Mexico|Distrito Federal
MH - Peoples R China
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 0
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0021-8693
UR - ISI:000088703000014
L2 - SPLIT-SEQUENCES; REPRESENTATION THEORY; ARTIN ALGEBRAS
SO - Journal of Algebra 2000 ;230(2):665-675
188
UI - 14598
AU - Bayro-Corrochano E
AU - Zhang YW
AD - Ctr Invest Matemat AC, Guanajuato 36000, MexicoUniv Kiel, Inst Comp Sci, D-24105 Kiel, GermanyBayro-Corrochano, E, Ctr Invest Matemat AC, Apartado Postal 402, Guanajuato 36000, Mexico
TI - The motor extended Kalman filter: A geometric approach for rigid motion estimation
AB - In this paper the motor algebra for linearizing the 3D Euclidean motion of lines is used as the oretical basis for the development of a novel extended Kalman filter called the motor extended Kalman filter (MEKF). Due to its nature the MEKF can be used as online approach as opposed to batch SVD methods. The MEKF does not encounter singularities when computing the Kalman gain and it can estimate simultaneously the translation and rotation transformations. Many algorithms in the literature compute the translation and rotation transformations separately. The experimental part demonstrates that the motor extended Kalman filter is an useful approach for estimation of dynamic motion problems. We compare the MEKF with an analytical method using simulated data. We present also an application using real images of a visual guided robot manipulator; the aim of this experiment is to demonstrate how we can use the online MEKF algorithm. After the system has been calibrated, the MEKF estimates accurately the relative position of the end-effector and a 3D reference line. We believe that future vision systems being reliably calibrated will certainly make great me of the MEKF algorithm
MH - Germany
MH - Mexico|Guanajuato
PB - DORDRECHT: KLUWER ACADEMIC PUBL
RP - NOT IN FILE
U3 - TC 3
U4 - Computer Science, Artificial Intelligence;Computer Science, Software Engineering;Mathematics, Applied
U5 - J;Article
AV - English
IS - 0924-9907
UR - ISI:000166111700004
L2 - computer vision;Clifford algebra;geometric algebra;kinematics;dynamics;rotors;motors;screws;Kalman filter techniques;extended Kalman filter;visual robotics;ATTITUDE
SO - Journal of Mathematical Imaging and Vision 2000 ;13(3):205-228
189
UI - 14686
AU - Bayro-Corrochano E
AU - Daniilidis K
AU - Sommer G
AD - Ctr Invest Matemat, Guanajuato 36000, MexicoUniv Penn, Grasp Lab, Philadelphia, PA 19104, USAUniv Kiel, Inst Comp Sci, D-24105 Kiel, GermanyBayro-Corrochano, E, Ctr Invest Matemat, Apartado Postal 402, Guanajuato 36000, Mexico
TI - Motor algebra for 3D kinematics: The case of the hand-eye calibration
AB - In this paper we apply the Clifford geometric algebra for solving problems of visually guided robotics. In particular, using the algebra of motors we model the 3D rigid motion transformation of points, lines and planes useful for computer Vision and robotics. The effectiveness of the Clifford algebra representation is illustrated by the example of the hand-eye calibration. It is shown that the problem of the hand-eye calibration is equivalent to the estimation of motion of lines. The authors developed a new linear algorithm which estimates simultaneously translation and rotation as components of rigid motion
MH - Germany
MH - Mexico|Guanajuato
MH - USA
PB - DORDRECHT: KLUWER ACADEMIC PUBL
RP - NOT IN FILE
U3 - TC 9
U4 - Computer Science, Artificial Intelligence;Computer Science, Software Engineering;Mathematics, Applied
U5 - J;Article
AV - English
IS - 0924-9907
UR - ISI:000165905300001
L2 - computer vision;kinematics;visual robotics;Clifford algebra;geometric algebra;rotors;motors;screws;hand-eye calibration;ROBOT MANIPULATORS; TRANSFORMATIONS; QUATERNIONS; MATRICES; SENSOR
SO - Journal of Mathematical Imaging and Vision 2000 ;13(2):79-100
190
UI - 15399
AU - Bayro-Corrochano E
AU - Kahler D
AD - Ctr Invest Matemat, Guanajuato, Gto, MexicoUniv Kiel, Inst Comp Sci, D-24105 Kiel, GermanyBayro-Corrochano, E, Ctr Invest Matemat, AC Apartado Postal 402, Guanajuato, Gto, Mexico
TI - Motor algebra approach for computing the kinematics of robot manipulators
AB - This article presents the formulation of the robot manipulator kinematics in the geometric algebra framework. In this algebraic system the three-dimensional Euclidean motion of points, lines, and planes can be advantageously represented using the algebra of motors. The computational complexity of the direct and indirect kinematics and other problems concerning robot manipulators depend on their degrees of freedom as well as on their geometric characteristics. Our approach makes possible a direct algebraic formulation of the problem in such a way that it reflects the underlying geometric structure. This is achieved by switching where necessary to a description of parts of the problem based on motor representations of points, lines, and planes. This article presents the formulation and computation of closed-form solutions of the direct and indirect kinematics of standard robot manipulators and a simple example of a grasping task. The flexible method presented here is new, and it widens the current standard point or line representation-based approaches for the treatment of problems related to robot manipulators. (C) 2000 John Wiley gr Sons, Inc
MH - Germany
MH - Mexico|Guanajuato
PB - NEW YORK: JOHN WILEY & SONS INC
RP - NOT IN FILE
U3 - TC 3
U4 - Robotics
U5 - J;Article
AV - English
IS - 0741-2223
UR - ISI:000088830200004
L2 - MATRICES
SO - Journal of Robotic Systems 2000 ;17(9):495-516
191
UI - 14226
AU - Bea RG
AU - Valle O
AD - Univ Calif Berkeley, Dept Civil & Environm Engn, Berkeley, CA 94720, USAInst Mexicano Petr, Mexico City 07730, DF, MexicoBea, RG, Univ Calif Berkeley, Dept Civil & Environm Engn, 212 McLaughlin Hall, Berkeley, CA 94720 USA
TI - Key issues associated with development of reassessment and requalification criteria for platforms in the Bay of Campeche, Mexico
AB - Petroleos Mexicano (PEMEX) and Institute Mexicano del Petroleo (IMP) have developed and issued Transitory Criteria for reassessment and requalification of platforms and pipelines in the Bay of Campeche (1998). The purpose of this paper is to highlight some of the key issues that were associated with development of the PEMEX-IMP guidelines and to identify some of the future efforts that are intended to extend the technology of platform reassessment and requalifications. It is hoped that the open exchange and discussion of this experience will help promote worldwide cooperation and development of this important technology. [S0892-7219(00)00801-3]
MH - USA
MH - Mexico|Distrito Federal
PB - NEW YORK: ASME-AMER SOC MECHANICAL ENG
RP - NOT IN FILE
U3 - TC 0
U4 - Engineering, Ocean;Engineering, Mechanical
U5 - J;Article
AV - English
IS - 0892-7219
UR - ISI:000167107000003
SO - Journal of Offshore Mechanics and Arctic Engineering-Transactions of the Asme 2000 ;122(1):7-19
192
UI - 16574
AU - Becker V
AU - Tapia M
AU - Alvarez R
AU - Gonzalez-Serratos H
AU - Ortega A
AD - Univ Nacl Autonoma Mexico, Fac Med, Dept Bioquim, Mexico City 04510, DF, MexicoUniv Maryland, Sch Med, Dept Physiol, College Pk, MD 20742, USA
TI - Muscle adaption to exercise, changes the Ca2+-pump activities from T-Tubule and sarcoplasmic reticulum membranes
MH - Mexico|Distrito Federal
MH - USA
PB - BETHESDA: BIOPHYSICAL SOCIETY
RP - NOT IN FILE
U3 - TC 0
U4 - Biophysics
U5 - J;Meeting Abstract
AV - English
IS - 0006-3495
UR - ISI:000084779302549
SO - Biophysical Journal 2000 ;78(1):436A-436A
193
UI - 15267
AU - Behle RW
AU - McGuire MR
AU - Tamez-Guerra P
AD - USDA ARS, Natl Ctr Agr Utilizat Res, Bioact Agents Res Unit, Peoria, IL 61604, USAUANL, Dept Microbiol & Inmunol, Fac Ciencias Biol, San Nicolas Garza 66450, NL, MexicoBehle, RW, USDA ARS, Natl Ctr Agr Utilizat Res, Bioact Agents Res Unit, 1815 N Univ St, Peoria, IL 61604 USA
TI - Effect of light energy on alkali-released virions from Anagrapha falcifera nucleopolyhedrovirus
AB - We compared the insecticidal activities of occluded and nonoccluded AfMNPV baculovirus obtained by dissolving the occlusion bodies (OB) with sodium carbonate. Droplet feeding and cotton leaf feeding bioassay techniques were used to determine the dose response against neonate Trichoplusia ni (Hubner) and loss of insecticidal activity when the virus was exposed to simulated sunlight from a xenon light source. Using droplet bioassays to determine a dose response, nonoccluded virus (NOV) was 20 times more active (LC50 = 4.8 x 10(3) OB/ml, dissolved) than occluded virus (LC50 = 9.6 x 10(4) OB/ml) when the samples remained wet. However, NOV lost activity when air dried before being tested by droplet (LC50 > 1.0 x 10(6) OB/ml) or leaf feeding (LC50 > 3.0 x 10(6) OB/ml) bioassays. Adding sucrose to NOV prevented the loss of insecticidal activity when samples were dried. The activity of NOV with 2% sucrose was similar to that of occluded virus samples, with or without sucrose, in both droplet feeding and leaf feeding assays. These results indicate that the OB protected the insecticidal activity of virions from the detrimental effects of drying. The OB also provided some protection from the detrimental effects of simulated sunlight (xenon) exposure. NOV samples exposed to xenon light had significantly greater loss of insecticidal activity than did similar samples of occluded virus. Without advancement in technologies, such as formulations, possible benefits of increased insecticidal activity from the use of nonoccluded virus is probably not sufficient to offset the rapid loss of activity due to drying or light exposure. (C) 2000 Academic Press
MH - USA
MH - Mexico|Nuevo Leon
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 6
U4 - Zoology
U5 - J;Article
AV - English
IS - 0022-2011
UR - ISI:000089301200005
L2 - NUCLEAR POLYHEDROSIS-VIRUS; SIMULATED SUNLIGHT-UV; AUTOGRAPHA-CALIFORNICA; FORMULATIONS; BACULOVIRUS
SO - Journal of Invertebrate Pathology 2000 ;76(2):120-126
194
UI - 16523
AU - Beitia C
AU - Borensztein Y
AU - Barrera RG
AU - Roman-Velazquez CE
AU - Noguez C
AD - Univ Paris 06, Lab Opt Solides, F-75252 Paris 05, FranceUniv Nacl Autonoma Mexico, Inst Fis, Mexico City 01000, DF, MexicoBorensztein, Y, Univ Paris 06, Lab Opt Solides, Case 80,4 Pl Jussieu, F-75252 Paris 05, France
TI - Multipolar plasma resonances in supported alkali-metal nanoparticles
AB - Multipolar effects in the polarizability of metallic potassium particles on a silicon substrate were studied using differential reflectance spectroscopy. The experimental spectra were compared with calculations of the effective polarizability of particles of different shapes leading to the conclusion that the resonances in the spectra correspond to excitations of substrate-induced multipolar modes in the particle-substrate system. (C) 2000 Elsevier Science B.V. All rights reserved
MH - France
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 2
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0921-4526
UR - ISI:000085314700008
L2 - multipole plasmon;metal particles;ADSORBED OVERLAYERS; TRUNCATED SPHERE; POLARIZABILITY; SUBSTRATE; REFLECTANCE
SO - Physica B-Condensed Matter 2000 ;279(1-3):25-28
195
UI - 15279
AU - Beligiannis A
AD - Natl Autonomous Univ Mexico, Inst Matemat, Mexico City 04510, DF, MexicoBeligiannis, A, Univ Aegean, Dept Math, Karlovassi 83200, Samos, Greece
TI - The homological theory of contravariantly finite subcategories: Auslander-Buchweitz contexts, Gorenstein categories and (CO-)stabilization
MH - Greece
MH - Mexico|Distrito Federal
PB - NEW YORK: MARCEL DEKKER INC
RP - NOT IN FILE
U3 - TC 16
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0092-7872
UR - ISI:000089301000002
L2 - TRIANGULATED CATEGORIES; FLAT COVERS; MODULES; ALGEBRAS
SO - Communications in Algebra 2000 ;28(10):4547-4596
196
UI - 15086
AU - Belkova NV
AU - Bakhmutova EV
AU - Shubina ES
AU - Bianchini C
AU - Peruzzini M
AU - Bakhmutov VI
AU - Epstein LM
AD - AN Nesmeyanov Organoelement Cpds Inst, Moscow 117813, RussiaCNR, Ist Studio Stereochim & Energet Composti Coor, I-50132 Florence, ItalyIPN, Dept Chem, Ctr Invest & Estud Avanzados, Mexico City 07000, DF, MexicoBianchini, C, AN Nesmeyanov Organoelement Cpds Inst, Vavilovstr 28, Moscow 117813, Russia
TI - The energy profile of proton transfer from Bronsted acids to terminal hydrides in transition metal complexes can be estimated by combining in situ IR and NMR spectroscopy
AB - The enthalpy and entropy changes relative to the stepwise reaction of [(triphos)Re(CO)(2)H] with perfluoro-tert-butyl alcohol in CH2Cl2 to give first the hydrogen-bonded adduct [(triphos)Re(CO)(2)H...HOC(CF3)(3)] and then the stable nonclassical dibydrogen complex [(triphos)Re(CO)(2)(eta(2)-H-2)](+) have been estimated by a combination of in situ IR and NMR experiments in the temperature range from 200 to 260 K [triphos = MeC(CH2PPh2)(3)]
MH - Italy
MH - Mexico|Distrito Federal
MH - Russia
PB - BERLIN: WILEY-V C H VERLAG GMBH
RP - NOT IN FILE
U3 - TC 15
U4 - Chemistry, Inorganic & Nuclear
U5 - J;Article
AV - English
IS - 1434-1948
UR - ISI:000089837900004
L2 - hydrides;hydrogen bonding;rhenium;IR spectroscopy;NMR spectroscopy;DOT-H-OR; DIHYDROGEN COMPLEXES; HYDROGEN; KINETICS; DONORS
SO - European Journal of Inorganic Chemistry 2000 ;(10):2163-2165
197
UI - 14972
AU - Ben Youssef C
AU - Guillou V
AU - Olmos-Dichara A
AD - Inst Politecn Nacl, Ctr Invest Computac, Unidad Profes Adolfo Lopez Mateos, Mexico City 07738, DF, MexicoCNRS, UMR 5504, Ctr Bioingn Gilbert Durand, F-31077 Toulouse 4, FranceINRA, Inst Natl Sci Appl, F-31077 Toulouse 4, FranceUniv Autonoma Metropolitana Iztapalapa, Dept Biotecnol, Mexico City 09340, DF, MexicoBen Youssef, C, Inst Politecn Nacl, Ctr Invest Computac, Unidad Profes Adolfo Lopez Mateos, Calle Juan Dios Batiz S-N,Col Nueva Ind Vallejo, Mexico City 07738, DF, Mexico
TI - Modelling and adaptive control strategy in a lactic fermentation process
AB - The modelling and design of an adaptive control strategy for lactic acid production in a continuous-flow two-stage reactor is reported. First, the medium enrichment effect, only recently investigated, is explicitly taken into account to derive an experimental model validated in batch cultures. Then, the control objective, which relies on a trade-off between total substrate depletion and optimal productivity, is stated according to economic imperatives of lactic acid production optimisation. A preliminary steady-state analysis allows the control objective to be formulated in terms of substrate supply regulation. Due to the practical importance of achieving applicable control, an adaptive-multivariable predictive-control law, where only the process output is needed and where the specific rate parameters are considered as time-varying, is proposed. Evaluation by simulation shows the efficiency and feasibility of such a control system. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - France
MH - Mexico|Distrito Federal
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 1
U4 - Automation & Control Systems;Engineering, Electrical & Electronic
U5 - J;Article
AV - English
IS - 0967-0661
UR - ISI:000165081600008
L2 - process modelling;adaptive control;multivariable control;process parameter estimation;fermentation process;LACTOBACILLUS-HELVETICUS; PREDICTIVE CONTROL; ACID PRODUCTION; WHEY PERMEATE; CELL-RECYCLE; LACTATE FERMENTATION; CONTINUOUS CULTURE; YEAST EXTRACT; BATCH CULTURE; GROWTH
SO - Control Engineering Practice 2000 ;8(11):1297-1307
198
UI - 14751
AU - Benet L
AU - Izrailev FM
AU - Seligman TH
AU - Suarez-Moreno A
AD - UNAM, Ctr Ciencias Fis, Cuernavaca, Morelos, MexicoCtr Int Ciencias, Cuernavaca, Morelos, MexicoBUAP, Inst Fis, Puebla 72570, MexicoUNAM, Inst Fis, Mexico City, DF, MexicoBenet, L, Max Planck Inst Kernphys, D-69117 Heidelberg, Germany
TI - Semiclassical properties of eigenfunctions and occupation number distribution for a model of two interacting particles
AB - Quantum-classical correspondence for the shape of eigenfunctions, local spectral density of states and occupation number distribution is studied in a chaotic model of two coupled quartic oscillators. In particular, it is shown that both classical quantities and quantum spectra determine global properties of occupation numbers and inverse participation ratio. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Germany
MH - Mexico|Distrito Federal
MH - Mexico|Morelos
MH - Mexico|Puebla
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 12
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0375-9601
UR - ISI:000165728100005
L2 - eigenfunction shape;local density of states;inverse participation ratio;quantum-classical correspondence;FINITE FERMI SYSTEMS; STATISTICAL-THEORY; STATES; CHAOS; SPACE; THERMALIZATION
SO - Physics Letters A 2000 ;277(2):87-93
199
UI - 15256
AU - Benet L
AU - Seligman TH
AD - UNAM, Ctr Ciencias Fis, Cuernavaca, Morelos, MexicoCtr Int Ciencias, Cuernavaca, Morelos, MexicoBenet, L, Max Planck Inst Kernphys, Postfach 103980, D-69117 Heidelberg, Germany
TI - Generic occurrence of rings in rotating systems
AB - In rotating scattering systems, the generic saddle-center scenario leads to stable islands in phase space. Non-interacting particles whose initial conditions are defined in such islands will be trapped and form rotating rings. This result is generic and also holds for systems quite different from planetary rings. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Germany
MH - Mexico|Morelos
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 6
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0375-9601
UR - ISI:000089283700008
L2 - rings;rotating scattering systems;stable orbits;saddle-center bifurcations;CHAOTIC SCATTERING; SATURN
SO - Physics Letters A 2000 ;273(5-6):331-337
200
UI - 14846
AU - Benintende GB
AU - Lopez-Meza JE
AU - Cozzi JG
AU - Piccinetti CF
AU - Ibarra JE
AD - Inst Nacl Tecnol Agropecuaria, Inst Microbiol & Zool Agricola, RA-1712 Castelar, ArgentinaUniv Michoacana, Ctr Multidisciplinario Estud Biotecnol, Morelia, Michoacan, MexicoIPN, Ctr Invest & Estudios Avanzados, Dept Biotecnol & Bioquim, Irapuato 36500, Guanajuato, MexicoBenintende, GB, Inst Nacl Tecnol Agropecuaria, Inst Microbiol & Zool Agricola, CC 25, RA-1712 Castelar, Argentina
TI - Characterization of INTA 51-3, a new atypical strain of Bacillus thuringiensis from Argentina
AB - Several isolates of Bacillus thuringiensis native to Argentina obtained in a nationwide screening program showed atypical crystal morphology. One of these strains, INTA 51-3, was further characterized in order to determine other features like protein composition of its parasporal crystal, plasmid pattern, identification of cry genes and toxicological properties. B. thuringiensis INTA 51-3 (serovar tohokuensis) had an amorphous inclusion containing a major protein component of cn. 130 kDa. After trypsin digestion of solubilized crystals, SDS-PAGE resolved a unique protease-resistant peptide of ca. 90 kDa. The plasmid pattern from INTA 51-3 resembled that of the standard strain HD-1. However, Southern analysis showed no hybridization to fragments of cry1Aa, cry2Aa, cry3A, and cry11A genes. Degenerate primers were used for identification of the cry1 genes by PCR. Nevertheless, the presence of cry1 type gene(s) in B. thuringiensis INTA 51-3 was confirmed. Highly concentrated crystal suspensions showed to be weakly toxic only to lepidopteran species
MH - Argentina
MH - Mexico|Guanajuato
MH - Mexico|Michoacan
PB - NEW YORK: SPRINGER-VERLAG
RP - NOT IN FILE
U3 - TC 5
U4 - Microbiology
U5 - J;Article
AV - English
IS - 0343-8651
UR - ISI:000165497400005
L2 - LARVICIDAL ACTIVITY; CRYSTAL PROTEINS; INSECTS
SO - Current Microbiology 2000 ;41(6):396-401
201
UI - 15693
AU - Benz BF
AU - Cevallos J
AU - Santana F
AU - Rosales J
AU - Graf S
AD - Texas Wesleyan Univ, Dept Biol, Ft Worth, TX 76105, USAUniv Guadalajara, Inst Manantlan Ecol & Conservac Biodiversidad, Autlan 48900, Jalisco, MexicoInst Nacl Ecol Secretario Medio Ambiente, Direcc Reserva Biosfera Sierra Manantlan, Autlan 48900, Jalisco, MexicoBenz, BF, Texas Wesleyan Univ, Dept Biol, Ft Worth, TX 76105, USA
TI - Losing knowledge about plant use in the Sierra de Manantlan biosphere reserve, Mexico
AB - The purpose of this paper is to document relationships between knowledge of plant use and indicators of modernization in Mexico. The model we are resting envisions increasing loss of plant use knowledge with increasing modernization indicated by loss of indigenous language and acquisition of nontraditional community services such as literacy and quality of housing. As predicted, we demonstrate that empirical knowledge about plant use is both more diverse and more evenly shared by people speaking an indigenous language - the Huastec - than by mestizo and Spanish-speaking indigenous populations in the Sierra de Manantlan. Our analyses also indicate that the adoption of modern community services by eight rural communities in the Sierra de Manantlan of western Mexico has had notable effects eroding traditional knowledge about useful plants in some but not all communities. From this we suggest that even though traditional knowledge about plants probably suffered a decline that accompanied loss of the indigenous language in Manantlan, traditional knowledge may be able to survive the modernization process today where such knowledge has an important role in subsistence
MH - Mexico|Jalisco
MH - USA
PB - BRONX: NEW YORK BOTANICAL GARDEN
RP - NOT IN FILE
U3 - TC 28
U4 - Plant Sciences
U5 - J;Article
AV - English
IS - 0013-0001
UR - ISI:000088062600009
L2 - ethnobotany;erosion of cultural knowledge;Sierra de Manantlan;Mexico;socioeconomic marginality;INDIGENOUS KNOWLEDGE; HYPOTHESES; FOREST
SO - Economic Botany 2000 ;54(2):183-191
202
UI - 15248
AU - Beran DD
AU - Masters RA
AU - Gaussoin RE
AU - Rivas-Pantoja F
AD - Univ Nebraska, USDA ARS, Lincoln, NE 68583, USAUniv Nebraska, Dept Agron, Lincoln, NE 68583, USAUniv Nebraska, Dept Hort, Lincoln, NE 68583, USAInst Nacl Invest Forestales & Agropecuarias, Merida, Yucatan, MexicoMasters, RA, Univ Nebraska, USDA ARS, Lincoln, NE 68583, USA
TI - Establishment of big bluestem and Illinois bundleflower mixtures with imazapic and imazethapyr
AB - Weeds interfere with establishment of native grasses and legumes. A study was conducted to determine the influence of imazapic(1) [(+/-)-2-[4,5-dihydro-4-methyl-4-(1-methylethyl)-5-oxo-1H-imidazol-2-yl] -5-methyl-3-pyridinecarboxylic acid] and imazethapyr [2-[4,5-dihydro-4-methyl-4-(1-methylethyl)-5-oxo-1H-imidazol-2-yl]5-ethy l-3-pyridinecarboxylic acid] on weed control and establishment of 'Pawnee' big bluestem (Andropogon gerardii Vitman var. gerardii Vitman) and Illinois bundleflower [Desmanthus illinoensis (Michx,) MacMill.] planted in three binary mixtures of 220:110, 165:165, and 110:220 pure live seed (PLS) m(-2). Mixtures were seeded st cropland sites near Clay Center, Mead, and Lincoln, NE. Imazapic and imazethapyr were applied at 70 g a.i. ha(-1) before planted species emerged. Imazapic or imazethapyr did not reduce dry matter yields of annual grass weeds, where herbicides were applied in April 1996 at Mead and Clay Center. Both grass and broadleaf weeds were controlled at Lincoln, where herbicides were applied in early June 1996, The herbicides usually improved big bluestem yields and total forage yields in 1996 and 1997 at all sites. Illinois bundleflower yields at Lincoln, where imazapic and imazethapyr were applied, were greater than 3.0 Mg ha(-1) in 1996 and 1997. In 1997, Illinois bundleflower did not survive at Mead and yielded less than 0.5 Mg ha(-1) at Clay Center, regardless of weed control treatment or seed mixture. Imazapic and imazethapyr can improve the establishment of big bluestem and Illinois bundleflower mixtures
MH - Mexico|Yucatan
MH - USA
PB - MADISON: AMER SOC AGRONOMY
RP - NOT IN FILE
U3 - TC 12
U4 - Agronomy
U5 - J;Article
AV - English
IS - 0002-1962
UR - ISI:000089408000010
L2 - SWITCHGRASS; HERBICIDES; CULTIVARS; ATRAZINE; PRAIRIE; YIELD
SO - Agronomy Journal 2000 ;92(3):460-465
203
UI - 14758
AU - Bergamin JM
AU - Bountis T
AU - Jung C
AD - Univ Patras, Dept Math, Patras 26500, GreeceUniv Patras, Ctr Applicat Nonlinear Syst, Patras 26500, GreeceUniv Nacl Autonoma Mexico, Ctr Ciencias Fis, Cuernavaca 62251, Morelos, MexicoBergamin, JM, Univ Patras, Dept Math, Patras 26500, Greece
TI - A method for locating symmetric homoclinic orbits using symbolic dynamics
AB - In this paper we present a method which can identify and locate symmetric homoclinic orbits in a homoclinic tangle formed by the intersecting stable and unstable manifolds of a symmetric 2D map. The method consists of a systematic search in parameter space and determination of the order in which these orbits arise using symbolic dynamics. Each orbit corresponds to a unique sequence and it is computed by iterating the map along the unstable manifold to match a specific symmetry at the middle of the orbit. An application of the method to the determination of multibreather solutions of 1D lattices is discussed
MH - Greece
MH - Mexico|Morelos
PB - BRISTOL: IOP PUBLISHING LTD
RP - NOT IN FILE
U3 - TC 6
U4 - Physics, Multidisciplinary;Physics, Mathematical
U5 - J;Article
AV - English
IS - 0305-4470
UR - ISI:000165753400008
L2 - NONLINEAR SCHRODINGER-EQUATION; WEAKLY COUPLED OSCILLATORS; INTRINSIC LOCALIZED MODES; SOLITON-LIKE SOLUTIONS; DISCRETE BREATHERS; NUMERICAL COMPUTATION; HAMILTONIAN NETWORKS; LINEAR-STABILITY; SYSTEMS; EXISTENCE
SO - Journal of Physics A-Mathematical and General 2000 ;33(45):8059-8070
204
UI - 15177
AU - Bergues JM
AU - Betancourt-Riera R
AU - Riera R
AU - Marin JL
AD - Sonoma State Univ, Dept Fis, Hermosillo 83000, Sonora, MexicoUniv Oriente, Dept Fis, Santiago, CubaUniv Sonora, Ctr Invest Fis, Hermosillo 83190, Sonora, MexicoBergues, JM, Sonoma State Univ, Dept Fis, Apartado Postal 1626, Hermosillo 83000, Sonora, Mexico
TI - One-phonon-assisted electron Raman scattering in quantum well wires and free-standing wires
AB - The differential cross section for an electron Raman scattering process in a semiconductor quantum well wire (QWW) and in a free-standing wire of cylindrical geometry involving phonon-assisted transitions is calculated for T = 0 K. A complete description of the phonon modes of cylindrical structures embedded in another material, including a correct treatment of the mechanical and electrostatic matching conditions at the surface, is presented We consider the Frohlich interaction to illustrate the theory for a GaAs/AlAs system. Electron states are considered to be confined within a QWW with finite and infinite potential barriers. We also assume single parabolic conduction and valence bands. The emission spectra are discussed for different scattering Configurations and the selection rules for the processes; are also studied. Singularities in the spectra are found and interpreted
MH - Cuba
MH - Mexico|Sonora
PB - BRISTOL: IOP PUBLISHING LTD
RP - NOT IN FILE
U3 - TC 12
U4 - Physics, Condensed Matter
U5 - J;Article
AV - English
IS - 0953-8984
UR - ISI:000089474700014
L2 - POLAR-OPTICAL OSCILLATIONS; GAAS-ALAS SUPERLATTICES; SEMICONDUCTOR SUPERLATTICES; MODES; DOTS; PHOTOLUMINESCENCE; FIELD
SO - Journal of Physics-Condensed Matter 2000 ;12(36):7983-7998
205
UI - 15148
AU - Berkove E
AU - Farrell FT
AU - Juan-Pineda D
AU - Pearson K
AD - Lafayette Coll, Dept Math, Easton, PA 18042, USASUNY Binghamton, Dept Math, Binghamton, NY 13902, USAInst Matemat, Morelia 58089, Michoacan, MexicoUniv Valparaiso, Dept Math & Comp Sci, Valparaiso, IN 46383, USABerkove, E, Lafayette Coll, Dept Math, Easton, PA 18042, USA
TI - The Farrell-Jones Isomorphism Conjecture for finite covolume hyperbolic actions and the algebraic K-theory of Bianchi groups
AB - We prove the Farrell-Jones Isomorphism Conjecture for groups acting properly discontinuously via isometries on(real) hyperbolic n-space H-n with finite volume orbit space. We then apply this result to show that, for any Bianchi group Gamma, Wh(Gamma), (K) over tilde(0)(Z Gamma), and K-i(Z Gamma) vanish for i less than or equal to -1
MH - Mexico|Michoacan
MH - USA
PB - PROVIDENCE: AMER MATHEMATICAL SOC
RP - NOT IN FILE
U3 - TC 7
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0002-9947
UR - ISI:000089544700011
L2 - K-theory;discrete groups;MAPS
SO - Transactions of the American Mathematical Society 2000 ;352(12):5689-5702
206
UI - 15815
AU - Berman GP
AU - Doolen GD
AU - Lopez GV
AU - Tsifrinovich VI
AD - Univ Calif Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545, USAUniv Calif Los Alamos Natl Lab, CNLS, Los Alamos, NM 87545, USAUniv Guadalajara, Dept Fis, Guadalajara 44430, Jalisco, MexicoPolytech Univ, IDS Dept, Brooklyn, NY 11201, USABerman, GP, Univ Calif Los Alamos Natl Lab, Div Theoret, Los Alamos, NM 87545 USA
TI - Simulations of quantum-logic operations in a quantum computer with a large number of qubits
AB - We report the simulations of the dynamics of quantum-logic operations with large number of qubits (up to 1000). A nuclear-spin chain in which selective excitations of spins are provided by the gradient of the external magnetic field is considered. The spins interact with their nearest neighbors. We simulate the quantum controlled-Nor (CN) gate implementation for remote qubits, which provides the long-distance entanglement. Our approach can be applied to any implementation of quantum-logic gates involving a large number of qubits
MH - USA
MH - Mexico|Jalisco
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 12
U4 - Optics;Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 1050-2947
UR - ISI:000087567900024
L2 - SPIN-DIFFUSION; LATTICE; COMPUTATION; DYNAMICS
SO - Physical Review A 2000 ;6106(6):
207
UI - 16187
AU - Berman GP
AU - Doolen GD
AU - Lopez GV
AU - Tsifrinovich VI
AD - Univ Calif Los Alamos Natl Lab, CNLS, Div Theoret, Los Alamos, NM 87545, USAUniv Guadalajara, Dept Fis, Guadalajara 44430, Jalisco, MexicoPolytech Univ, IDS Dept, Brooklyn, NY 11201, USABerman, GP, Univ Calif Los Alamos Natl Lab, CNLS, Div Theoret, POB 1663, Los Alamos, NM 87545 USA
TI - Nonresonant effects in the implementation of the quantum Shor algorithm
AB - We simulate Shor's algorithm using the Ising spin quantum computer. The influence of nonresonant effects is analyzed in detail. It is shown that the method developed earlier in our papers successfully suppresses nonresonant effects even for relatively large values of the Rabi frequency
MH - Mexico|Jalisco
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 3
U4 - Optics;Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 1050-2947
UR - ISI:000086313300029
L2 - COMPUTATION; COMPUTER
SO - Physical Review A 2000 ;6104(4):
208
UI - 16491
AU - Berman GP
AU - James DFV
AU - Hughes RJ
AU - Gulley MS
AU - Holzscheiter MH
AU - Lopez GV
AD - Univ Calif Los Alamos Natl Lab, Grp T13, Los Alamos, NM 87545, USAUniv Calif Los Alamos Natl Lab, CNLS, Los Alamos, NM 87545, USAUniv Calif Los Alamos Natl Lab, Grp T4, Los Alamos, NM 87545, USAUniv Calif Los Alamos Natl Lab, Grp P23, Los Alamos, NM 87545, USAUniv Calif Los Alamos Natl Lab, Grp P25, Los Alamos, NM 87545, USAUniv Guadalajara, Dept Fis, Guadalajara 44420, Jalisco, MexicoBerman, GP, Univ Calif Los Alamos Natl Lab, Grp T13, POB 1663, Los Alamos, NM 87545 USA
TI - Dynamical stability and quantum chaos of ions in a linear trap
AB - The realization of a paradigm chaotic system, namely, the harmonically driven oscillator, in the quantum domain using cold trapped ions driven by lasers is theoretically investigated. The simplest characteristics of regular and chaotic dynamics are calculated. The possibilities of experimental realization are discussed
MH - Mexico|Jalisco
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 7
U4 - Optics;Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 1050-2947
UR - ISI:000085336900082
L2 - KICKED HARMONIC-OSCILLATOR; NONLINEAR RESONANCE; DIFFUSION; SYSTEMS; STATE; ATOM
SO - Physical Review A 2000 ;6102(2):
209
UI - 14800
AU - Bermudez M
AU - Montanez C
AU - Gomez P
AU - Yaffe D
AU - Cisneros B
AD - CINVESTAV IPN, Dept Genet & Mol Biol, Mexico City 07360, DF, MexicoWeizmann Inst Sci, Dept Cell Biol, IL-76100 Rehovot, Israel
TI - The Dp71 promoter activity is down-regulated during muscle cell differentiation
MH - Israel
MH - Mexico|Distrito Federal
PB - CHICAGO: UNIV CHICAGO PRESS
RP - NOT IN FILE
U3 - TC 0
U4 - Genetics & Heredity
U5 - J;Meeting Abstract
AV - English
IS - 0002-9297
UR - ISI:000089400701047
SO - American Journal of Human Genetics 2000 ;67(4):195-195
210
UI - 15357
AU - Bernal-Alvarado J
AU - Vargas-Luna M
AU - Solorza-Feria O
AU - Mondragon R
AU - onso-Vante N
AD - Univ Guanajuato, Inst Fis, Leon 37000, Gto, MexicoInst Politecn Nacl, CINVESTAV, Dept Quim, Mexico City 07000, DF, MexicoUniv Poitiers, Lab Electrocatalysis, CNRS, UMR 6503, F-86022 Poitiers, FranceBernal-Alvarado, J, Univ Guanajuato, Inst Fis, AP E-143, Leon 37000, Gto, Mexico
TI - Photoacoustic characterization of n-RuSe2 semiconductor pellets
AB - Using the open photoacoustic cell technique, a set of physical properties for a semiconductor (n-RuSe2) in powder form was measured. According to the Dramicanin theoretical model, charge carriers transport parameters (bulk and surface) and the effective thermal diffusivity were obtained. (C) 2000 American Institute of Physics. [S0021- 8979(00)08317-1]
MH - France
MH - Mexico|Distrito Federal
MH - Mexico|Guanajuato
PB - MELVILLE: AMER INST PHYSICS
RP - NOT IN FILE
U3 - TC 2
U4 - Physics, Applied
U5 - J;Article
AV - English
IS - 0021-8979
UR - ISI:000089034700098
L2 - TRANSPORT; CRYSTAL; SYSTEM; RUSE2
SO - Journal of Applied Physics 2000 ;88(6):3771-3772
211
UI - 14896
AU - Bernal-Uruchurtu MI
AU - Ruiz-Lopez MF
AD - Univ Nancy 1, UMR CNRS UHP 7565, Chim Theor Lab, F-54506 Vandoeuvre Les Nancy, FranceUniv Autonoma Estado Morelos, Ctr Invest Quim, Morelos, MexicoRuiz-Lopez, MF, Univ Nancy 1, UMR CNRS UHP 7565, Chim Theor Lab, BP 239, F-54506 Vandoeuvre Les Nancy, France
TI - Basic ideas for the correction of semiempirical methods describing H-bonded systems
AB - In this Letter, we show how semiempirical methods may be improved to describe hydrogen-bonded systems and proton transfer reactions. The approach consists in a redefinition of the core-core interaction terms that, as previously shown, are at the origin of spurious artifacts in standard methods. The parameterization of the new core-core functions is done using ab initio data of the intermolecular potential energy surfaces (PESs), which permits reaching the correct behavior at short and long interatomic distances. Here we report the parameters for O-O, O-H and H-H interactions. Extension to other atom pairs seems feasible, so the development of a semiempirical method adapted to the study of intermolecular interactions might be envisaged. (C) 2000 Elsevier Science B.V. All rights reserved
MH - France
MH - Mexico|Morelos
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 27
U4 - Chemistry, Physical;Physics, Atomic, Molecular & Chemical
U5 - J;Article
AV - English
IS - 0009-2614
UR - ISI:000165249100018
L2 - WATER; MODEL; AM1
SO - Chemical Physics Letters 2000 ;330(1-2):118-124
212
UI - 16113
AU - Bernal-Uruchurtu MI
AU - Martins-Costa MTC
AU - Millot C
AU - Ruiz-Lopez MF
AD - Univ Nancy 1, CNRS, UMR 7656, Chim Theor Lab,UHP,Inst Nanceien Chim Mol, F-54506 Vandoeuvre Nancy, FranceUniv Autonoma Estado Morelos, Ctr Invest Quim, Cuernavaca, Morelos, MexicoRuiz-Lopez, MF, Univ Nancy 1, CNRS, UMR 7656, Chim Theor Lab,UHP,Inst Nanceien Chim Mol, BP 239, F-54506 Vandoeuvre Nancy, France
TI - Improving description of hydrogen bonds at the semiempirical level: Water-water interactions as test case
AB - Hydrogen bonding is not well described by available semiempirical theories. This is an important restriction because hydrogen bonds represent a key feature in many chemical and biochemical processes, besides being responsible for the singular properties of water. In this study, we describe a possible solution to this problem. The basic idea is to replace the nonphysical gaussian correction functions (GCF) appearing in the core-core repulsion terms of most MNDO-based semiempirical methods by a simple function exhibiting the correct physical behavior in the whole range of intermolecular separation distances. The parameterized interaction function (PIF) is the sum of atom-pair contributions, each one having five adjustable parameters. In this work, the approach is used to study water-water interactions. The parameters are optimized to reproduce a reference ab initio intermolecular energy surface for the water-water dimer obtained at the MP2/aug-cc-pVQZ level. OO, OH, and HH parameters are reported for the PM3 method. The results of PMS-PIF calculations remarkably improve qualitatively and quantitatively those obtained at the standard PM3 level, both for water-dimer properties and for water clusters up to the hexamer. For example, the root-mean-square deviation of the PM3-PIF interaction energies, with respect to ab initio values obtained using 700 paints of the water dimer surface, is only 0.47 kcal/mol. This value is much smaller than that obtained using the standard PM3 method (4.2 kcal/mol). The PM3-PLF water dimer energy minimum ( 5.0 kcal/mol) is also much closer to ab initio data ( 5.0 +/- 0.01 kcal/mol) than PM3 ( 3.50 kcal/mol). The method is therefore promising for the development of new semiempirical approaches as well as for application of combined quantum mechanics and molecular mechanicstechniques to investigate chemical processes in water. (C) 2000 John Wiley & Sons, Inc
MH - France
MH - Mexico|Morelos
PB - NEW YORK: JOHN WILEY & SONS INC
RP - NOT IN FILE
U3 - TC 32
U4 - Chemistry, Multidisciplinary
U5 - J;Article
AV - English
IS - 0192-8651
UR - ISI:000086677400006
L2 - molecular interactions;hydrogen bonds;semiempirical methods;parameterizable interaction function;water dimer;AB-INITIO CALCULATIONS; CONFORMATIONAL-ANALYSIS; BINDING-ENERGIES; CORE-REPULSION; BASIS-SETS; CAGE FORM; CLUSTERS; DIMER; HEXAMER; SPECTRA
SO - Journal of Computational Chemistry 2000 ;21(7):572-581
213
UI - 16324
AU - Bernal J
AU - Harmony T
AU - Rodriguez M
AU - Reyes A
AU - Yanez G
AU - Fernandez T
AU - Galan L
AU - Silva J
AU - Fernandez-Bouzas A
AU - Rodriguez H
AU - Guerrero V
AU - Marosi E
AD - Univ Nacl Autonoma Mexico, ENEP Iztacala, Lab Neurometria Proy Neurociencias, Mexico City, DF, MexicoCtr Neurosci, La Habana, CubaBernal, J, Univ Nacl Autonoma Mexico, ENEP Iztacala, Lab Neurometria Proy Neurociencias, Manuel Fernando Soto 68,Col Constituc Republ, Mexico City, DF, Mexico
TI - Auditory event-related potentials in poor readers
AB - Although poor readers (PR) are considered the major group among reading-disabled children, there are not event-related potentials (ERP) studies reported of PR on the subject. In this study, attentional and memory processes were studied in an auditory oddball task in PR and normal controls. ERP to auditory stimuli were recorded in 19 leads of the 10/20 system, using linked earlobes as references, in 20 normal children (10 female) and 20 PR (10 female) of the same age(10-12 years old). Two pure tones (1000 and 3000 Hz) were used in an oddball paradigm. No significant differences were observed in the amplitudes and latencies of N100 between the groups. However, N200 to frequent stimuli and P200 to both frequent and infrequent stimuli were of higher amplitude in poor readers than in normal children. There were no differences between groups in the latency and amplitude of P300. The results suggest that PR use more attentional resources in the components occurring before P300 to both frequent and infrequent stimuli than the normal children, and this finding is particularly marked for PR girls. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Cuba
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 16
U4 - Psychology, Biological;Neurosciences;Physiology;Psychology;Psychology, Experimental
U5 - J;Article
AV - English
IS - 0167-8760
UR - ISI:000085978200002
L2 - P300;auditory event-related potentials;poor readers;reading disabilities;sex differences;DEVELOPMENTAL DYSLEXIA; WORKING-MEMORY; BRAIN POTENTIALS; CHILDREN; ATTENTION; DYSFUNCTIONS; ADULTS; BOYS; P300; DISABILITIES
SO - International Journal of Psychophysiology 2000 ;36(1):11-23
214
UI - 15958
AU - Beron-Vera FJ
AU - Ripa P
AD - Ctr Invest Cient & Educ Super Ensenada, Dept Oceanog Fis, Ensenada, Baja California, MexicoBeron-Vera, FJ, CICESE, Dept Phys Oceanog, POB 434844, San Diego, CA 92143 USA
TI - Three-dimensional aspects of the seasonal heat balance in the Gulf of California
AB - Previously unresolved three-dimensional aspects of the time mean, as well as the annual and semiannual cycles of the heat transport, ari studied in the Gulf of California using a minimal box model suggested by the hydrographic data. At the very least three horizontal domains are needed for the model a shallow region north of the big islands, a deep region identifiable with the Ballenas Channel, and another deep region spanning the rest of the gulf south of the archipelago. Only one vertical layer is considered in the northern region, whereas two layers are taken into account in the other two regions. Out of all of the possible heat exchanges among the various boxes of the model, the least-flux-variance solution is considered. The annual mean heat entering the surface in the northern region is exported in almost equal amounts to the Ballenas Channel and the southern region. Ballenas Channel, in turn, exports heat to the southern region mainly through the lower layer, producing a transversal asymmetry of the mouthward flux into the upper layer. At the mouth the heat is exported to the Pacific Ocean largely through the upper layer. Both the annual and semiannual amplitude of the exchanges between all regions are as important as the annual average, except at the mouth of the gulf, where the semiannual component is not statistically relevant. The Pacific Ocean fluxes estimates at the annual frequency agree well with those produced by a baroclinic wave, which has been shown to explain a bit; deal of the thermodynamics of the gulf. The annual mean vertical flux per unit horizontal area in the Ballenas Channel is much larger than that in the southern region. This reinforces previous speculations that mixing processes in this region are very important. A depth-independent eddy diffusivity parameterization suggests that diffusion might not be invoked to explain the annual, mean vertical flux in the Ballenas Channel
MH - USA
MH - Mexico|Baja California
PB - WASHINGTON: AMER GEOPHYSICAL UNION
RP - NOT IN FILE
U3 - TC 13
U4 - Oceanography
U5 - J;Article
AV - English
IS - 0148-0227
UR - ISI:000087153000014
L2 - OF-CALIFORNIA; VARIABILITY
SO - Journal of Geophysical Research-Oceans 2000 ;105(C5):11441-11457
215
UI - 15994
AU - Berrocal-Tito GM
AU - Rosales-Saavedra T
AU - Herrera-Estrella A
AU - Horwitz BA
AD - Technion Israel Inst Technol, Dept Biol, IL-32000 Haifa, IsraelIPN, Ctr Invest & Estud Avanzados, Dept Plant Genet Engn, Irapauto, MexicoHorwitz, BA, Technion Israel Inst Technol, Dept Biol, IL-32000 Haifa, Israel
TI - Characterization of blue-light and developmental regulation of the photolyase gene phr1 in Trichoderma harzianum
AB - Blue light and development regulate the expression of the phr1 gene of the filamentous fungus Trichoderma harzianum. The predicted product of phr1, the DNA repair enzyme photolyase, is likely to help protect Trichoderma, which grows in the soil as a mycoparasite or saprophyte, from damage upon emergence and exposure to ultraviolet-c, phr1 is transiently expressed in mycelium and conidiophores after illumination, phr1 mRNA also accumulates in conidiophores during development and spore maturation. As no other genes displaying rapid, direct Light regulation have been described previously in this organism, we have characterized the fluence and time dependence of phr1 induction, and its relation to sporulation and photoreactivation, Induction is transient following a pulse, and, with slower decay, in continuous Light. This implies that the photoreceptor, transducers or response are capable of adaptation. About two-fold more light is required to induce phr1 than conidiation, but this difference is modest, so both responses could use the same or similar chromophore. Adenosine 3':5'-cyclic monophosphate bypasses the requirement for light for sporulation, while atropine prevents sporulation even after photoinduction, Light regulation of phr1, however, is indifferent to both these effecters. Induction of photolyase expression behaves as a direct, rapid response to light, independent of the induction of sporulation. Indeed, illumination of mature spores increases their capacity for photoreactivation, Blue Light seems to warn the organism against the harmful effects of short wavelengths, inducing phr1 expression and sporulation by pathways that are, at least in part, distinct
MH - Israel
MH - Mexico|Guanajuato
PB - AUGUSTA: AMER SOC PHOTOBIOLOGY
RP - NOT IN FILE
U3 - TC 13
U4 - Biochemistry & Molecular Biology;Biophysics
U5 - J;Article
AV - English
IS - 0031-8655
UR - ISI:000086989700022
L2 - PYRIMIDINE DIMER PHOTOLYASE; PROTEINASE-ENCODING GENE; CULTURED FISH CELLS; NEUROSPORA-CRASSA; DIFFERENTIAL REGULATION; PHOTORECEPTOR; CRYPTOCHROME; EXPRESSION; INDUCTION; PHOTOREACTIVATION
SO - Photochemistry and Photobiology 2000 ;71(5):662-668
216
UI - 14663
AU - Berrocal M
AU - Ball AS
AU - Huerta S
AU - Barrasa JM
AU - Hernandez M
AU - Perez-Leblic MI
AU - Arias ME
AD - Univ Alcala, Dept Microbiol & Parasitol, Madrid 28871, SpainUniv Essex, Dept Biol Sci, Colchester CO4 3SQ, Essex, EnglandUniv Autonoma Metropolitana Iztapalapa, Dept Biotechnol, Mexico City 55535, DF, MexicoUniv Alcala, Dept Biol Vegetal, Madrid 28871, SpainArias, ME, Univ Alcala, Dept Microbiol & Parasitol, Madrid 28871, Spain
TI - Biological upgrading of wheat straw through solid-state fermentation with Streptomyces cyaneus
AB - The biological upgrading of wheat straw with Streptomyces cyaneus was examined through the analysis of chemical and structural changes of the transformed substrate during solid-state fermentation. Analysis of enzymes produced during the growth of S. cyaneus showed that phenol oxidase was the predominant enzyme. The reduction in Klason lignin content (16.4%) in the transformed substrate indicated the ability of this strain to delignify lignocellulose residues and suggests a role for phenol oxidase in the bacterial delignification process. Microscopic examination of the transformed substrate showed that the initial attack occurred at the less lignified cell walls (phloem and parenchyma), while xylem and sclerenchyma were slowly degraded. The pattern of degradation of sclerenchymatic tissues by S. cyaneus showed delamination between primary and secondary walls and between S-1 and S-2 due to partial removal of lignin. In the later stages of the decay a disorganization of the secondary walls was detected on account of fibrillation of this layer. A comparison of the properties of the pulp from wheat straw transformed by S. cyaneus with untreated wheat straw showed that pretreatment improved the characteristics that determine the quality of pulp. This was indicated by an increase in pulp brightness and by a decrease in the kappa number. These changes occurred without significantly affecting the viscosity, a measure of the quality of the cellulose fibres. These results support the potential application of this organism or its oxidative enzymes in biopulping
MH - United Kingdom
MH - Mexico|Distrito Federal
MH - Spain
PB - NEW YORK: SPRINGER-VERLAG
RP - NOT IN FILE
U3 - TC 7
U4 - Biotechnology & Applied Microbiology
U5 - J;Article
AV - English
IS - 0175-7598
UR - ISI:000166044200005
L2 - PHANEROCHAETE-CHRYSOSPORIUM; CERIPORIOPSIS-SUBVERMISPORA; ULTRASTRUCTURAL ASPECTS; LIGNIN; LIGNOCELLULOSE; SOLUBILIZATION; DEGRADATION; PULP; MINERALIZATION; PAPERMAKING
SO - Applied Microbiology and Biotechnology 2000 ;54(6):764-771
217
UI - 16231
AU - Berumen S
AU - Tiab D
AU - Rodriguez F
AD - PEMEX E&P, Coyoacan 04510, MexicoUniv Nacl Autonoma Mexico, Coyoacan 04510, MexicoUniv Oklahoma, Sch Petr & Geol Engn, Norman, OK 73019, USABerumen, S, PEMEX E&P, Ciudad Univ,Postal 70-256, Coyoacan 04510, Mexico
TI - Constant rate solutions for a fractured well with an asymmetric fracture
AB - This paper presents solutions for the pressure response on hydraulically fractured wells flowing at constant flow rate through an asymmetric vertical fracture. The pressure behavior of wells intercepting asymmetric fractures of both infinite and finite conductivity was investigated by solving numerically and analytically the mathematical model. The new solutions developed for the dimensionless wellbore pressure under production at constant flow rate are presented in terms of an asymmetry factor xi. New curves for these systems were generated and the deviation from the classical solution was readily detected. Some qualitative criteria to interpret the intensity of this effect are provided. Results of our investigation indicated that at early times for fractures of moderate conductivity (C-D < 5) the characteristic slope of one fourth is present, except for cases of strong asymmetry (0.85 < xi less than or equal to 1) where no evidence of straight line having one fourth slope was observed. However, it was also detected that at intermediate fracture conductivities (5 < C-D < 50), even the case of complete asymmetry shows the characteristic slope of one fourth. It was also observed that as the asymmetry factor increases, the end of the bilinear flow occurs earlier. Our results are relevant in improving the fracture characterization of fractured wells. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Mexico|Distrito Federal
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 0
U4 - Engineering, Petroleum;Geosciences, Multidisciplinary
U5 - J;Article
AV - English
IS - 0920-4105
UR - ISI:000086313000005
L2 - petroleum engineering;fracture conductivity;pressure analysis;asymmetric fractures;constant rate
SO - Journal of Petroleum Science and Engineering 2000 ;25(1-2):49-58
218
UI - 14891
AU - Besana A
AU - Rocchetti M
AU - Gurrola GB
AU - Zaza A
AD - Univ Milano Bicocca, Dipartimento Biotecnol & Biosci, Milan, ItalyUniv Nacl Autonoma Mexico, Inst Biotecnol, Cuernavaca 62191, Morelos, Mexico
TI - Rate-dependency of IKr and IKs during the ventricular action potential: implications for the mechanism of "reverse use-dependency"
MH - Italy
MH - Mexico|Morelos
PB - LONDON: W B SAUNDERS CO LTD
RP - NOT IN FILE
U3 - TC 0
U4 - Cardiac & Cardiovascular Systems
U5 - J;Meeting Abstract
AV - English
IS - 0195-668X
UR - ISI:000089136600242
SO - European Heart Journal 2000 ;21():63-63
219
UI - 15993
AU - Beuschel T
AU - Hirsch JG
AU - Draayer JP
AD - Louisiana State Univ, Dept Phys & Astron, Baton Rouge, LA 70803, USAUniv Nacl Autonoma Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoBeuschel, T, Louisiana State Univ, Dept Phys & Astron, Baton Rouge, LA 70803 USA
TI - Scissors mode and the pseudo-SU(3) model
AB - The low-lying M1 transition strength distributions observed in rare earth and actinide nuclei reflects on both the collective and noncollective aspects of the nuclear interaction. As shown in this article, the pseudo-SU(3) model can accommodate these complementary features and provides a natural interpretation for different aspects of this "scissors" mode
MH - USA
MH - Mexico|Distrito Federal
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 9
U4 - Physics, Nuclear
U5 - J;Article
AV - English
IS - 0556-2813
UR - ISI:000086953000019
L2 - MAGNETIC DIPOLE EXCITATIONS; DEFORMED-NUCLEI; SHELL-MODEL; SCATTERING
SO - Physical Review C 2000 ;6105(5):
220
UI - 16482
AU - Bhalekar AA
AD - Nagpur Univ, Dept Chem, Nagpur 440010, Maharashtra, IndiaUAM, Iztapalapa, MexicoIACS, Calcutta, W Bengal, India
TI - On the irreversible thermodynamic framework for closed systems consisting of chemically reactive components
AB - A methodology has been described to develop an irreversible thermodynamic framework based on the laws of thermodynamics and exemplified by applying it to a spatially uniform chemically reacting closed system with no irreversibility in the energy exchanges. It is shown thar if in the Gibbs relation the chemical composition determining extensive parameters appear as independent thermodynamic variables and if their variation includes the changes due to chemical reaction, then it, in fact, is an irreversible thermodynamic description. The de Donderian thermodynamic framework is basically a nonequilibrium description in which the chemical affinity containing term is the manifestation of the irreversibility in chemical interactions. This confirms that the Gibbs function primarily takes care of the chemical interactions and hence the quantification of the irreversibility in the latter need to be achieved through the former function by identifying its suitable expression
MH - India
MH - Mexico|Distrito Federal
PB - SAHIBABAD: MRS PUSHPA AGARWAL
RP - NOT IN FILE
U3 - TC 3
U4 - Chemistry, Multidisciplinary
U5 - J;Article
AV - English
IS - 0970-7077
UR - ISI:000085448500020
L2 - NONEQUILIBRIUM TEMPERATURE; EXTENDED THERMODYNAMICS; TRANSPORT PROCESSES; REALITY; CHECK
SO - Asian Journal of Chemistry 2000 ;12(2):433-444
221
UI - 16035
AU - Bhaud M
AU - Fernandez-Alamo MA
AD - Univ Paris 06, CNRS, Observ Oceanol Banyuls, F-66651 Banyuls sur Mer, FranceUniv Nacl Autonoma Mexico, Fac Ciencias, Lab Invertebrados, Mexico City 04510, DF, MexicoBhaud, M, Univ Paris 06, CNRS, Observ Oceanol Banyuls, BP 44, F-66651 Banyuls sur Mer, France
TI - Planktonic larvae of Spiochaetopterus in the Gulf of California: New evidence that the geographic distribution of species with a long planktonic larval life is relatively restricted (Polychaeta, Chaetopteridae)
AB - Polychaete larvae were sorted fi-om a collection of 116 zooplankton samples taken in 76 localities during the GOLCA 84-04 cruise in March-April 1984. Two morphologies were identified in the Chaetopreridae genus Spiochaetopterus: larval types I and II. The morphology of A4 setae dissected from the larvae is compared with A4 setae of erected species from the Pacific. Larvae of Spiochaetopterus type I could belong to S. monroi. From local observation of adults and larvae, and comparison with the first species described in the genus: S. costarum, it appears that this species is not present in the Gulf of California. Although S. costarum was for a long time credited with a widespread distribution throughout the world because of its long planktonic larval development, it is now acknowledged that many reported occurrences were in-correctly attributed to S. costarum, and in consequence its specific area has been restricted ill recent years. This paper confirms that the setal morphology of larvae and adults is very helpful in the identification of planktonic larval stages
MH - France
MH - Mexico|Distrito Federal
PB - STENSTRUP: OPHELIA PUBLICATIONS
RP - NOT IN FILE
U3 - TC 4
U4 - Marine & Freshwater Biology
U5 - J;Article
AV - English
IS - 0078-5326
UR - ISI:000086898200007
L2 - Polychaeta;Chaetopteridae;Spiochaetopterus;larvae;Gulf of California
SO - Ophelia 2000 ;52(1):65-76
222
UI - 14804
AU - Bhutta ZA
AU - Bird SM
AU - Black RE
AU - Brown KH
AU - Gardner JM
AU - Hidayat A
AU - Khatun F
AU - Martorell R
AU - Ninh NX
AU - Penny ME
AU - Rosado JL
AU - Roy SK
AU - Ruel M
AU - Sazawal S
AU - Shankar A
AD - Johns Hopkins Sch Publ Hlth, Dept Int Hlth, Baltimore, MD 21205, USAAga Khan Univ, Med Ctr, Karachi 74800, PakistanMRC, Biostat Unit, Cambridge CB2 2BW, EnglandUniv Calif Davis, Davis, CA 95616, USAUniv W Indies, Mona, JamaicaTrisakti Univ, Jakarta, IndonesiaDhaka Med Coll, Dhaka, BangladeshEmory Univ, Atlanta, GA 30322, USANatl Inst Nutr, Hanoi, VietnamInst Nutr Res, Lima, PeruNatl Inst Nutr, Mexico City, DF, MexicoInt Ctr Diarrhoeal Dis Res, Dhaka 1000, BangladeshInst Nutr Cent Amer & Panama, Guatemala City, GuatemalaAll India Inst Med Sci, New Delhi, IndiaBlack, RE, Johns Hopkins Sch Publ Hlth, Dept Int Hlth, 615 N Wolfe St, Baltimore, MD 21205 USA
TI - Therapeutic effects of oral zinc in acute and persistent diarrhea in children in developing countries: pooled analysis of randomized controlled trials
AB - Background: Zinc deficiency is prevalent in children in developing countries. Supplemental zinc provides therapeutic benefits in diarrhea. Objective: We sought to measure the effect of supplemental zinc given with oral rehydration therapy during recovery from acute or persistent diarrhea. Design: We conducted pooled analyses including all available published and unpublished randomized controlled trials of the effects of supplementary oral zinc in children aged < 5 y with acute or persistent diarrhea. We used Cox survival regression analysis to evaluate the overall effect of zinc on continuation of diarrhea and possible differential effects in subgroups divided by sex, age, weight-for-height, and initial plasma zinc concentration. Dichotomous outcomes were analyzed by logistic regression. To assess the effects of excluding studies without original data from the pooled analyses, effect-size was estimated for all studies by using random-effects models. Results: Zinc-supplemented children had a 15% lower probability of continuing diarrhea on a given day (95% CI: 5%, 24%) in the acute-diarrhea trials and a 24% lower probability of continuing diarrhea (95% CI: 9%, 37%) and a 42% lower rate of treatment failure or death (95% CI: 10%, 63%) in the persistent-diarrhea trials. In none of the subgroup analyses were the 2 subgroups of each pair significantly different from each other; however, in persistent diarrhea there tended to be a greater effect in subjects aged < 12 mo, who were male, or who had wasting or lower baseline plasma zinc concentrations. Conclusion: Zinc supplementation reduces the duration and severity of acute and persistent diarrhea
MH - Bangladesh
MH - United Kingdom
MH - Guatemala
MH - India
MH - Indonesia
MH - Jamaica
MH - USA
MH - Mexico|Distrito Federal
MH - Pakistan
MH - Peru
MH - Vietnam
PB - BETHESDA: AMER SOC CLINICAL NUTRITION
RP - NOT IN FILE
U3 - TC 133
U4 - Nutrition & Dietetics
U5 - J;Article
AV - English
IS - 0002-9165
UR - ISI:000165549000018
L2 - diarrhea;diarrheal disease;malnutrition;meta-analysis;randomized controlled trial;zinc;children;infants;developing countries;zinc supplementation;nutrition;zinc deficiency;MALNOURISHED BANGLADESHI CHILDREN; YOUNG-CHILDREN; INTESTINAL PERMEABILITY; SUPPLEMENTATION; DEFICIENCY; INFANTS; MALNUTRITION; MAGNITUDE; INFECTION; PATTERNS
SO - American Journal of Clinical Nutrition 2000 ;72(6):1516-1522
223
UI - 15408
AU - Bianchi G
AU - Gislason H
AU - Graham K
AU - Hill L
AU - Jin X
AU - Koranteng K
AU - Manickchand-Heileman S
AU - Paya I
AU - Sainsbury K
AU - Sanchez F
AU - Zwanenburg K
AD - Inst Marine Res, N-5817 Bergen, NorwayDanish Inst Fisheries Res, Univ Copenhagen, DK-2920 Charlottenlund, DenmarkNew S Wales Fisheries Res Inst, Cronulla, NSW, AustraliaIPIMAR, Lisbon, PortugalMarine Fisheries Res Div, Tema, GhanaNatl Autonomous Univ Mexico, Inst Marine Sci & Limnol, Mexico City 04510, DF, MexicoInst Fomento Pesquero, Valparaiso, ChileCSIRO, Marine Lab, Hobart, Tas 7001, AustraliaINIDEP, Mar Del Plata, ArgentinaYellow Sea Fishery Res Inst, Qingdao, Peoples R ChinaBedford Inst Oceanog, Marine Fish Div, Dartmouth, NS, CanadaBianchi, G, Inst Marine Res, POB 1870 Nordnes, N-5817 Bergen, Norway
TI - Impact of fishing on size composition and diversity of demersal fish communities
AB - By analysing data sets from different world regions we add evidence to documented changes in demersal fish community structure that may be related to fishing. Changes are analysed by community properties that might be expected to capture relevant overall changes - size spectra slopes and intercepts, Shannon-Wiener diversity, and dominance. Cross-system differences in the shape of the integrated community size spectra appear to be related to ecosystem productivity. The slope of size spectra appears to respond in a consistent way to changes in exploitation levels. In most areas studied. but particularly in high-latitude regions, we observe a decreasing trend in the slope, reflecting changes in size composition toward a relative decline in larger fish. The results from tropical regions are less conclusive, partly owing to the difficulty in obtaining consistent data series, but probably also because the generally higher growth rates of the constituent species make the slope less sensitive to changes in fishing. No evidence was found of any decline in species richness, while changes in diversity (richness and evenness) were caused either by changes in patterns of dominance or by changes in the number of species identified resulting from improved survey protocols. (C) 2000 International Council for the Exploration of the Sea
MH - Argentina
MH - Australia
MH - Canada
MH - Chile
MH - Denmark
MH - Ghana
MH - Mexico|Distrito Federal
MH - Norway
MH - Peoples R China
MH - Portugal
PB - LONDON: ACADEMIC PRESS LTD
RP - NOT IN FILE
U3 - TC 72
U4 - Fisheries;Marine & Freshwater Biology;Oceanography
U5 - J;Article
AV - English
IS - 1054-3139
UR - ISI:000088880200012
L2 - cross-system comparisons;diversity;fish community structure;size spectrum;NORTH-SEA; LONG-TERM; ASSEMBLAGES; SPECTRA; SHELF; GULF; CARPENTARIA; AUSTRALIA; ABUNDANCE; ATLANTIC
SO - Ices Journal of Marine Science 2000 ;57(3):558-571
224
UI - 14662
AU - Bicay MD
AU - Stepanian JA
AU - Chavushyan VH
AU - Erastova LK
AU - Ayvazyan VT
AU - Seal J
AU - Kojoian G
AD - Russian Acad Sci, Special Astrophys Observ, Karachai Cherkessia 357147, RussiaCALTECH, Jet Prop Lab, Pasadena, CA 91109, USAInst Nacl Astrofis Opt Elect, Puebla 72000, MexicoByurakan Astrophys Observ, Byurakan, ArmeniaArmenian State Pedag Inst, Dept Phys & Astron, Yerevan 375010, ArmeniaCambridge CR&D, Sidney, IL 61877, USAUniv Wisconsin, Dept Phys & Astron, Eau Claire, WI 54702, USAStepanian, JA, Russian Acad Sci, Special Astrophys Observ, Karachai Cherkessia 357147, Russia
TI - Accurate optical positions for 2978 objects from the Second Byurakan Survey (SBS) with the Digitized Sky Survey
AB - Optical positions of 2978 objects listed in the Second Byurakan Survey (SBS) were obtained using the Digitized Sky Survey (DSS), and are given with an rms uncertainty similar to1 arcsec in each coordinate
MH - Armenia
MH - Mexico|Puebla
MH - Russia
MH - USA
PB - LES ULIS CEDEXA: E D P SCIENCES
RP - NOT IN FILE
U3 - TC 17
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0365-0138
UR - ISI:000166021400001
L2 - surveys;catalogs : active;galaxies;quasars;FINDING CHARTS; GALAXIES; QUASARS; SYSTEM
SO - Astronomy & Astrophysics Supplement Series 2000 ;147(2):169-173
225
UI - 14936
AU - Bichet D
AU - Lecomte C
AU - Sabatier JM
AU - Felix R
AU - De Waard M
AD - Fac Med Nord, Inst Fed Jean Roche, INSERM U464, Lab Neurobiol Canaux Ion, F-13916 Marseille 20, FranceFac Med Nord, Inst Fed Jean Roche, CNRS, UMR 6560,Lab Biochim, F-13916 Marseille, FranceIPN, CINVESTAV, Dept Physiol Biophys & Neurosci, Mexico City 0700, DF, MexicoBichet, D, Fac Med Nord, Inst Fed Jean Roche, INSERM U464, Lab Neurobiol Canaux Ion, Blvd Pierre Dramard, F-13916 Marseille 20, France
TI - Reversibility of the Ca2+ channel alpha(1)-beta subunit interaction
AB - The auxiliary beta subunit importantly regulates voltage-dependent Ca2+ channel activity through an interaction with the AID domain, a binding site located in the cytoplasmic I-II linker of the ion-conducting alpha (1) subunit. In the present study, we used two synthetic peptides corresponding to partial. sequences of the I-II linker of alpha (1A) (AID(A)-peptides) as tools to disrupt the alpha (1)-beta interaction. In vitro binding experiments confirmed that these peptides exhibit a reasonable affinity to the neuronal beta (3) subunit to serve this purpose, although they failed to prevent immunoprecipitation of native N- and P/Q-type channels by anti-beta (3) antibodies. Together, our results (i) provide evidence for the reversibility of channel subunit association suggesting that the disruption of the alpha (1)-beta interaction may be a possible mechanism for Ca2+ channel regulation in vivo, and (ii) support a model whereby the alpha (1)-beta association is based on multiple interaction sites. (C) 2000 Academic Press
MH - France
MH - Mexico|Distrito Federal
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 15
U4 - Biochemistry & Molecular Biology;Biophysics
U5 - J;Article
AV - English
IS - 0006-291X
UR - ISI:000165214500035
L2 - Ca2+ channel;alpha(1) subunit;beta subunit;subunit interaction;DEPENDENT CALCIUM CHANNELS; PROTEIN-COUPLED RECEPTORS; BETA-SUBUNIT; ALPHA(1A) SUBUNIT; IDENTIFICATION; ANTIBODIES; BINDING; COMPLEX; DOMAIN; GAMMA
SO - Biochemical and Biophysical Research Communications 2000 ;277(3):729-735
226
UI - 15288
AU - Bijker R
AU - Iachello F
AU - Leviatan A
AD - UNAM, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoYale Univ, Sloane Lab, Ctr Theoret Phys, New Haven, CT 06520, USAHebrew Univ Jerusalem, Racah Inst Phys, IL-91904 Jerusalem, IsraelBijker, R, UNAM, Inst Ciencias Nucl, AP 70-543, Mexico City 04510, DF, Mexico
TI - Algebraic models of hadron structure II. Strange baryons
AB - The algebraic treatment of baryons is extended to strange resonances. Within this framework we study a collective string-like model in which the radial excitations are interpreted as rotations and vibrations of the strings. We derive a mass formula and closed expressions for strong and electromagnetic decay widths and use these to analyze the available experimental data. (C) 2000 Academic Press
MH - Israel
MH - Mexico|Distrito Federal
MH - USA
PB - SAN DIEGO: ACADEMIC PRESS INC
RP - NOT IN FILE
U3 - TC 19
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0003-4916
UR - ISI:000089234800004
L2 - NONSTRANGE BARYONS; RADIATIVE DECAYS; QUARK-MODEL; SCATTERING; SPECTRA; ETA
SO - Annals of Physics 2000 ;284(1):89-133
227
UI - 15813
AU - Bijker R
AU - Iachello F
AD - Natl Autonomous Univ Mexico, Inst Ciencias Nucl, Mexico City 04510, DF, MexicoYale Univ, Sloane Lab, Ctr Theoret Phys, New Haven, CT 06520, USABijker, R, Natl Autonomous Univ Mexico, Inst Ciencias Nucl, Apartado Postal 70-543, Mexico City 04510, DF, Mexico
TI - Cluster states in nuclei as representations of a U(nu+1) group
AB - We propose a description of cluster states in nuclei in terms of representations of unitary algebras U(nu + 1), where nu is the number of space degrees of freedom. Within this framework, a variety of situations including both vibrational and rotational spectra, soft and rigid configurations, identical and nonidentical constituents can be described. As an example, we show how the method can be used to study alpha clustering configurations in C-12 With point group symmetry D-3h
MH - Mexico|Distrito Federal
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 5
U4 - Physics, Nuclear
U5 - J;Article
AV - English
IS - 0556-2813
UR - ISI:000087575000084
L2 - MOLECULAR-SPECTRA
SO - Physical Review C 2000 ;6106(6):
228
UI - 15517
AU - Binder T
AU - Cruse A
AU - Villar CAC
AU - Marquardt W
AD - Rhein Westfal TH Aachen, Lehrstuhl Prozesstech, D-52056 Aachen, GermanyCol San Pedro, Dept Ingn Elect, Zacatenco, MexicoBinder, T, Rhein Westfal TH Aachen, Lehrstuhl Prozesstech, Templegraben 55, D-52056 Aachen, Germany
TI - Dynamic optimization using a wavelet based adaptive control vector parameterization strategy
AB - In this work we present an adaptive parameterization strategy for the so-called sequential solution approach where the optimization problem is approximated by a nonlinear program (NLP) by parameterization of the control variables only. The proposed method is embedded into a solution methodology where a hierarchy of successively refined finite dimensional optimization problems are solved. Information on the solution of the coarser approximation is used to construct a fully adaptive, problem dependent parameterization. The adaptation is built on a multiscale setting involving wavelets. We demonstrate examplarily that the adaptive parameterization is more efficient and robust compared with a uniform parameterization of comparable accuracy. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Germany
MH - Mexico|Distrito Federal
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 8
U4 - Computer Science, Interdisciplinary Applications;Engineering, Chemical
U5 - J;Article
AV - English
IS - 0098-1354
UR - ISI:000088546800151
L2 - dynamic optimization;large scale systems;adaptive mesh refinement;control vector parameterization;single shooting;wavelets
SO - Computers & Chemical Engineering 2000 ;24(2-7):1201-1207
229
UI - 16056
AU - Binette L
AU - Kurk JD
AU - Villar-Martin M
AU - Rottgering HJA
AD - Univ Nacl Autonoma Mexico, Inst Astron, Mexico City 04510, DF, MexicoLeiden Observ, NL-2300 RA Leiden, NetherlandsUniv Hertfordshire, Dept Phys Sci, Hatfield AL10 9AB, Herts, EnglandBinette, L, Univ Nacl Autonoma Mexico, Inst Astron, Ap 70-264, Mexico City 04510, DF, Mexico
TI - A vestige low metallicity gas shell surrounding the radio galaxy 0943-242 at z=2.92
AB - Observations are presented showing the doublet C IV lambda lambda 1548, 1551 absorption lines superimposed on the C rv emission in the radio galaxy 0943-242. Within the errors, the redshift of the absorption system that has a column density of N-CIV = 10(14.5+/-0.1) cm(-2) coincides with that of the deep Ly alpha absorption trough observed by Rottgering et al. (1995). The gas seen in absorption has a resolved spatial extent of at least 13 kpc (the size of the extended emission line region). We first model the absorption and emission gas as co-spatial components with the same metallicity and degree of excitation. Using the information provided by the emission and absorption line ratios of C IV and Ly alpha, we find that the observed quantities are incompatible with photoionization or collisional ionization of cloudlets with uniform properties. We therefore reject the possibility that the absorption and emission phases are co-spatial and favour the explanation that the absorption gas has low metallicity and is located further away from the host galaxy (than the emission line gas). The larger size considered for the outer halo makes plausible the proposed metallicity drop relative to the inner emission gas. In absence of confining pressure comparable to that of the emission gas, the outer halo of 0943-242 is considered to have a very low density allowing the metagalactic ionizing radiation to keep it higly ionized. In other radio galaxies where the jet has pressurized the outer halo, the same gas would be seen in emission (since the emissivity scales as n(H)(2)) and not in absorption as a result of the lower filling factor of the denser condensations. This would explain the anticorrelation found by van Ojik et al. (1997) between Ly alpha emission sizes (or radio jet sizes) and the observation (or not) of H I in absorption. The estimated low metallicity for the absorption gas in 0943-242 (Z similar to 0.01Z.) and its proposed location -outer halo outside the radio cocoon-suggest that its existence preceeds the observed AGN phase and is a vestige of the initial starburst at the onset of formation of the parent galaxy
MH - United Kingdom
MH - Mexico|Distrito Federal
MH - Netherlands
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 23
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-6361
UR - ISI:000086869300011
L2 - galaxies : individual : 0943-242;cosmology : early Universe;galaxies : active;galaxies : formation;galaxies : ISM;ELEMENT ABSORPTION SYSTEMS; HIGH-REDSHIFT; EVOLUTION; SPECTRUM; CLOUDS
SO - Astronomy and Astrophysics 2000 ;356(1):23-32
230
UI - 14155
AU - Blanco-Davila F
AU - Luce EA
AD - Univ Neuvo Leon Hosp, Div Plast Surg, Monterrey, Neuvo Leon, MexicoCase Western Reserve Univ, Div Plast & Reconstruct Surg, Cleveland, OH 44106, USABlanco-Davila, F, Sexta Avenida 227,Col Cumbres, Monterrey, NL, Mexico
TI - Current considerations for myelomeningocele repair
AB - Important advances have been made in the reconstruction of myelomeningocele during the last few years. Techniques of closure that use diverse tissues available in the back range from very simple to very complex. Most of them have become essential to the plastic surgeon. To facilitate a more efficient interdisciplinary approach, recent advances in knowledge of the vascular anatomy of the skin and specific clinical surgical considerations concerning skin grafts, cutaneous flaps, and musculocutaneous flaps are reviewed. A topographical division of the lesion that will permit a methodologically adequate treatment plan for congenital defects in the back, specifically in the thoracic, thoracolumbar, and:lumbosacral regions is suggested
MH - Mexico|Nuevo Leon
MH - USA
PB - PHILADELPHIA: LIPPINCOTT WILLIAMS & WILKINS
RP - NOT IN FILE
U3 - TC 3
U4 - Surgery
U5 - J;Article
AV - English
IS - 1049-2275
UR - ISI:000167444800012
L2 - meningomyelocele;surgical flaps;blood supply;anatomy;spinal dysraphism;DORSI MYOCUTANEOUS FLAP; MUSCULOCUTANEOUS FLAP; MENINGOMYELOCELE DEFECTS; CHEST-WALL; CLOSURE; MUSCLE; SPINE
SO - Journal of Craniofacial Surgery 2000 ;11(5):500-508
231
UI - 16394
AU - Blazquez J
AU - Ruiz J
AD - CIEMAT, Dept Nucl Fiss, E-28040 Madrid, SpainRuiz, J, Natl Inst Nucl Res, Mexico City, DF, Mexico
TI - Neutron signal characterization of the power instability event at Laguna Verde BWR
AB - On January 24, 1995, a power instability event occurred in Laguna Verde, a BWR/5 commercial plant. Recorded power oscillations were studied from the point of view of noise analysis. The 723-s long recorded signal comes from average power range monitors and was bad conditioned for noise analysis practice; it was neither stationary in mean, nor in variance. The signal first stage corresponds to the stable reactor; the third stage, to the unstable reactor. There was a second intermediate stage regarded as a transition one. The signal was preconditioned and divided in small blocks. Noise was analysed within each block in the amplitude, frequency and time domains. The analysis was aimed at on early recognition of instability by using the noise to discriminate between stable, transition and unstable state, regardless of the domain chosen for analysis. The experience obtained from studying real events, not depending on any physical model, are the ground for making safer operation procedures. (C) 2000 Published by Elsevier Science S.A. All rights reserved
MH - Mexico|Distrito Federal
MH - Spain
PB - LAUSANNE: ELSEVIER SCIENCE SA
RP - NOT IN FILE
U3 - TC 2
U4 - Nuclear Science & Technology
U5 - J;Article
AV - English
IS - 0029-5493
UR - ISI:000085729300007
L2 - MODEL
SO - Nuclear Engineering and Design 2000 ;196(3):327-336
232
UI - 15281
AU - Blumenthal UJ
AU - Mara DD
AU - Peasey A
AU - Ruiz-Palacios G
AU - Stott R
AD - Univ London London Sch Hyg & Trop Med, Dept Infect & Trop Med, London WC1E 7HT, EnglandUniv Leeds, Sch Civil Engn, Leeds, W Yorkshire, EnglandLondon Sch Hyg & Trop Med, Dept Infect & Trop Dis, Mexico City, DF, MexicoNatl Inst Nutr, Dept Infect Dis, Mexico City, DF, MexicoUniv Portsmouth, Dept Civil Engn, Portsmouth, Hants, EnglandBlumenthal, UJ, Univ London London Sch Hyg & Trop Med, Dept Infect & Trop Med, Keppel St, London WC1E 7HT, England
TI - Guidelines for the microbiological quality of treated wastewater used in agriculture: recommendations for revising WHO guidelines
AB - Three different approaches for establishing guidelines for the microbiological quality of treated wastewater that is reused for agriculture are reviewed. These approaches have different objectives as their outcomes: the absence of faecal indicator organisms in the wastewater, the absence of a measurable excess of cases of enteric disease in the exposed population and a model-generated estimated risk below a defined acceptable risk. If the second approach (using empirical epidemiological studies supplemented by microbiological studies of the transmission of pathogens) is used in conjunction with the third approach (using a model-based quantitative risk assessment for selected pathogens) a powerful tool is produced that aids the development of regulations. This combined approach is more cost-effective than the first approach and adequately protects public health. The guideline limit for faecal coliform bacteria in unrestricted irrigation (less than or equal to 1000 faecal coliform bacteria/100 ml) is valid, but for restricted irrigation less than or equal to 10(5) faecal coliform bacteria/100 ml is recommended when adult farmworkers are exposed to spray irrigation. A limit of less than or equal to 10(3) faecal coliform bacteria/100 ml is recommended if flood irrigation is used or children are exposed. The guideline limit for nematode eggs for both types of irrigation is adequate except when conditions favour the survival of nematode eggs and where children are exposed; in these cases it should be reduced from less than or equal to 1 egg/l to less than or equal to 0.1 egg/l
MH - United Kingdom
MH - Mexico|Distrito Federal
PB - GENEVA 27: WORLD HEALTH ORGANIZATION
RP - NOT IN FILE
U3 - TC 36
U4 - Public, Environmental & Occupational Health
U5 - J;Article
AV - English
IS - 0042-9686
UR - ISI:000089263900005
L2 - water microbiology, standards;Enterobacteriaceae;maximum allowable concentration;agriculture;World Health Organization;guidelines;VIRUS MONITORING DATA; WATER RECLAMATION; RISK ASSESSMENT; STABILIZATION PONDS; SPRAY IRRIGATION; REUSE; CRYPTOSPORIDIUM; GIARDIA; DISEASE; REMOVAL
SO - Bulletin of the World Health Organization 2000 ;78(9):1104-1116
233
UI - 15285
AU - Bocardo JCE
AU - Ramirez MA
AU - Donizak J
AU - Kolenda Z
AD - IPN, Ctr Invest & Estudios Avanzados, Saltillo, Coahuila, MexicoAkad Gorniczo Hutnicza, Katedra Teorii & Inzynierii Proc Met, PL-30059 Krakow, PolandBocardo, JCE, IPN, Ctr Invest & Estudios Avanzados, Saltillo, Coahuila, Mexico
TI - Computer-aided cooling curve analysis applied to Co-Cr-Mo system
AB - Computer-aided cooling curve analysis has been applied to a cobalt-based alloy, (widely used in the production of surgical implants) resulting in better understanding of the solidification process, Transformation temperatures and latent heat of solidification have been evaluated. Further kinetics study of solidification has been made yielding information on the evolution of solid fraction during solidification process. Segregation patterns were obtained by means of metallographic and microanalysis techniques
MH - Mexico|Coahuila
MH - Poland
PB - KRAKOW: POLISH ACAD SCIENCES COMMITTEE METALLURGY
RP - NOT IN FILE
U3 - TC 1
U4 - Metallurgy & Metallurgical Engineering
U5 - J;Article
AV - English
IS - 0860-7052
UR - ISI:000089306700006
L2 - EQUIAXED DENDRITIC GROWTH; SOLUTE DIFFUSION-MODEL; SOLIDIFICATION
SO - Archives of Metallurgy 2000 ;45(2):185-196
234
UI - 16669
AU - Bogdanchikova N
AU - Petranovskii V
AU - Fuentes S
AU - Paukshtis E
AU - Sugi Y
AU - Licea-Claverie A
AD - UNAM, Ctr Ciencias Mat Condensada, San Ysidro, CA 92143, USACICESE, Ensenada 22800, Baja California, MexicoInst Catalysis, Novosibirsk 630090, RussiaGifu Univ, Gifu 50511, JapanInst Tecnol Tijuana, CGI, Tijuana 22000, BC, MexicoBogdanchikova, N, UNAM, Ctr Ciencias Mat Condensada, POB 439036, San Ysidro, CA 92143 USA
TI - Role of mordenite acid properties in silver cluster stabilization
AB - In the present work, the role of SiO2/Al2O3 molar ratio in silver cluster stabilization inside mordenite pores was studied. It was found that SiO2/Al2O3 molar ratio regulates silver cluster stabilization by means of change of mordenite acid properties. The high concentration and high strength of Bronsted acid sites favor the stabilization of silver in the form of clusters inside the pores. In contrast, low concentration and low strength of Bronsted acid sites and high concentration of Lewis sites inside the channels can hinder stabilization of silver clusters. In this case, large particles on the external surface of zeolite are preferably formed. It was revealed that silver cluster introduction in its turn influences acid properties of mordenites, changing the concentration and structure of acid sites. As a result of silver incorporation, four types of Lewis acid sites presented in H-mordenites disappear and a new type of Lewis acid site appears. For the majority of samples, it is accompanied by enhancement of concentration of Lewis sites so that all Al becomes 'IR visible'. (C) 2000 Elsevier Science S.A. All rights reserved
MH - USA
MH - Japan
MH - Mexico|Baja California
MH - Russia
PB - LAUSANNE: ELSEVIER SCIENCE SA
RP - NOT IN FILE
U3 - TC 14
U4 - Nanoscience & Nanotechnology;Materials Science, Multidisciplinary
U5 - J;Article
AV - English
IS - 0921-5093
UR - ISI:000084583200029
L2 - mordenite;acid properties;silver clusters
SO - Materials Science and Engineering A-Structural Materials Properties Microstructure and Processing 2000 ;276(1-2):236-242
235
UI - 16396
AU - Bohigas J
AU - Tapia M
AU - Ruiz MT
AU - Roth M
AD - UNAM, Inst Astron, Ensenada 2800, Baja California, MexicoUniv Chile, Dept Astron, Santiago, ChileCarnegie Inst Washington, Las Campanas Observ, La Serena, ChileBohigas, J, UNAM, Inst Astron, Apdo Postal 877, Ensenada 2800, Baja California, Mexico
TI - Possible detection of an old bipolar shell associated with eta Carinae
AB - Continuum-subtracted dereddened images in the light of several atomic lines show the presence of an extended bipolar nebula surrounding eta Carinae with size similar to 100 x 45 arcsec(2) (1.3 x 0.5 pc(2)). This feature is best delineated in [O III] 5007. The geometrical disposition and mass of the shell suggest that it was formed by mass ejections from eta Carinae, The dynamic age of the nebula is similar to 13 000/V-7 yr, where V-7 is the mean expansion velocity in 100 km s(-1), and its mass is between 5 and 10 M.. The nebula is photoionized and composed of unprocessed material. The major axes of the nebula and of the Homunculus are nearly perpendicular. We also report the discovery of elongated emission knots prominent in [N II] located 64 to 100 arcsec away from eta Carinae, which implies that they were ejected either centuries ago or at a more recent date bht with extremely large velocities
MH - Chile
MH - Mexico|Baja California
PB - OXFORD: BLACKWELL SCIENCE LTD
RP - NOT IN FILE
U3 - TC 10
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0035-8711
UR - ISI:000085823700009
L2 - stars : individual : eta Carinae;stars : variables : other;HII regions;ISM : individual : NGC 3372;LUMINOUS BLUE VARIABLES; AG-CARINAE; X-RAYS; NEBULAE; MORPHOLOGY; LBV
SO - Monthly Notices of the Royal Astronomical Society 2000 ;312(2):295-300
236
UI - 16608
AU - Bohm A
AU - Kaldass H
AU - Wickramasekara S
AU - Kielanowski P
AD - Univ Texas, Dept Phys, Austin, TX 78712, USAIPN, Dept Fis, Ctr Invest & Estudios Avanzados, Mexico City, DF, MexicoBohm, A, Univ Texas, Dept Phys, Austin, TX 78712, USA
TI - Semigroup representations of the Poincare group and relativistic Gamow vectors
AB - Gamow vectors are generalized eigenvectors (kets) of self-adjoint Hamiltonians with complex eigenvalues (E-R -/+ i Gamma/2) describing quasistable states. In the relativistic domain this leads to Poincare semigroup representations which are describing quasistable states. In the relativistic domain this leads to Poincare a characterized by spin j and by complex invariant mass square s = s(R) = ( M-R - 1/2 Gamma(R))(2). Relativistic Gamow kets have all the properties required to describe relativistic resonances and quasistable particles with resonance mass M-R and lifetime h/Gamma(R). (C) 2000 Published by Elsevier Science B.V. All rights reserved
MH - Mexico|Distrito Federal
MH - USA
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 10
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0375-9601
UR - ISI:000084914200001
L2 - Poincare semigroup;relativistic resonances;decaying states;IRREVERSIBILITY
SO - Physics Letters A 2000 ;264(6):425-433
237
UI - 16577
AU - Bombal F
AU - Fernandez M
AD - Univ Complutense Madrid, Dept Anal Matemat, Madrid, SpainCIMAT, Guanajuato, MexicoBombal, F, Univ Complutense Madrid, Dept Anal Matemat, Madrid, Spain
TI - Polynomial properties and symmetric tensor product of Banach spaces
AB - We study some classes of distinguished subsets of a Banach space in terms of polynomials and their relationship. This allows us to develop a systematic approach to study polynomial properties on a Banach space. We apply this approach to obtain several known and new results on the symmetric tensor product of a Banach space in a unified way
MH - Mexico|Guanajuato
MH - Spain
PB - BASEL: BIRKHAUSER VERLAG AG
RP - NOT IN FILE
U3 - TC 2
U4 - Mathematics
U5 - J;Article
AV - English
IS - 0003-889X
UR - ISI:000085111400007
SO - Archiv der Mathematik 2000 ;74(1):40-49
238
UI - 14871
AU - Bombardier C
AU - Laine L
AU - Reicin A
AU - Shapiro D
AU - Burgos-Vargas R
AU - Davis B
AU - Day R
AU - Ferraz MB
AU - Hawkey CJ
AU - Hochberg MC
AU - Kvien TK
AU - Schnitzer TJ
AU - Weaver A
AD - Mt Sinai Hosp, Inst Work & Hlth, Toronto, ON M5G 1X5, CanadaUniv Hlth Network, Toronto, ON, CanadaUniv So Calif, Sch Med, Dept Med, Gastrointestinal Div, Los Angeles, CA 90033, USAUniv Nacl Autonoma Mexico, Fac Med, Mexico City 04510, DF, MexicoUniv Nacl Autonoma Mexico, Div Res, Mexico City 04510, DF, MexicoMerck & Co Inc, Rahway, NJ 07065, USAHosp Gen Mexico, Mexico City, DF, MexicoUniv Texas, Sch Publ Hlth, Houston, TX, USAUniv New S Wales, Dept Clin Pharmacol, Sydney, NSW, AustraliaSt Vincents Hosp, Sydney, NSW 2010, AustraliaUniv Fed Sao Paulo, Escola Paulista Med, Dept Med, Div Rheumatol, Sao Paulo, BrazilUniv Nottingham Hosp, Sch Med & Surg Sci, Div Gastroenterol, Nottingham NG7 2UH, EnglandUniv Maryland, Div Clin Immunol & Rheumatol, Baltimore, MD 21201, USAOslo City Dept Rheumatol, Oslo, NorwayDiakonhjemmet Hosp, Oslo, NorwayNorthwestern Univ, Sch Med, Off Clin Res & Training, Chicago, IL, USABombardier, C, Inst Work & Hlth, 250 Bloor St E,Suite 702, Toronto, ON M4W 1E6, Canada
TI - Comparison of upper gastrointestinal toxicity of rofecoxib and naproxen in patients with rheumatoid arthritis
AB - Background: Each year, clinical upper gastrointestinal events occur in 2 to 4 percent of patients who are taking nonselective nonsteroidal antiinflammatory drugs (NSAIDs). We assessed whether rofecoxib, a selective inhibitor of cyclooxygenase-2, would be associated with a lower incidence of clinically important upper gastrointestinal events than is the nonselective NSAID naproxen among patients with rheumatoid arthritis. Methods: We randomly assigned 8076 patients who were at least 50 years of age (or at least 40 years of age and receiving long-term glucocorticoid therapy) and who had rheumatoid arthritis to receive either 50 mg of rofecoxib daily or 500 mg of naproxen twice daily. The primary end point was confirmed clinical upper gastrointestinal events (gastroduodenal perforation or obstruction, upper gastrointestinal bleeding, and symptomatic gastroduodenal ulcers). Results: Rofecoxib and naproxen had similar efficacy against rheumatoid arthritis. During a median follow-up of 9.0 months, 2.1 confirmed gastrointestinal events per 100 patient-years occurred with rofecoxib, as compared with 4.5 per 100 patient-years with naproxen (relative risk, 0.5; 95 percent confidence interval, 0.3 to 0.6; P<0.001). The respective rates of complicated confirmed events (perforation, obstruction, and severe upper gastrointestinal bleeding) were 0.6 per 100 patient-years and 1.4 per 100 patient-years (relative risk, 0.4; 95 percent confidence interval, 0.2 to 0.8; P=0.005). The incidence of myocardial infarction was lower among patients in the naproxen group than among those in the rofecoxib group (0.1 percent vs. 0.4 percent; relative risk, 0.2; 95 percent confidence interval, 0.1 to 0.7); the overall mortality rate and the rate of death from cardiovascular causes were similar in the two groups. Conclusions: In patients with rheumatoid arthritis, treatment with rofecoxib, a selective inhibitor of cyclooxygenase-2, is associated with significantly fewer clinically important upper gastrointestinal events than treatment with naproxen, a nonselective inhibitor. (N Engl J Med 2000;343:1520-8.) (C) 2000, Massachusetts Medical Society
MH - Australia
MH - Brazil
MH - Canada
MH - United Kingdom
MH - Mexico|Distrito Federal
MH - Norway
MH - USA
PB - WALTHAM: MASSACHUSETTS MEDICAL SOC
RP - NOT IN FILE
U3 - TC 1621
U4 - Medicine, General & Internal
U5 - J;Article
AV - English
IS - 0028-4793
UR - ISI:000165410900003
L2 - NONSTEROIDAL ANTIINFLAMMATORY DRUGS; DOUBLE-BLIND; CONTROLLED TRIAL; CYCLOOXYGENASE; OSTEOARTHRITIS; COMPLICATIONS; INHIBITION; CELECOXIB
SO - New England Journal of Medicine 2000 ;343(21):1520-1528
239
UI - 16654
AU - Bonvicini V
AU - Busso L
AU - Giubellino P
AU - Gregorio A
AU - Idzik M
AU - Kolojvari A
AU - Montano LM
AU - Nouais D
AU - Petta C
AU - Rashevsky A
AU - Randazzo N
AU - Reito S
AU - Tosello F
AU - Vacchi A
AU - Vinogradov L
AU - Zampa N
AD - Ist Nazl Fis Nucl, Sez Trieste, Trieste, ItalyIst Nazl Fis Nucl, Sez Torino, I-10125 Turin, ItalyIst Nazl Fis Nucl, Sez Catania, I-95129 Catania, ItalyAcad Min & Met, Fac Phys & Nucl Tech, Krakow, PolandSt Petersburg State Univ, Cyclotron Lab, St Petersburg, RussiaCINVESTAV, Mexico City 14000, DF, MexicoBonvicini, V, Ist Nazl Fis Nucl, Sez Trieste, Trieste, Italy
TI - Laboratory and test beam results from a large-area silicon drift detector
AB - A very large-area (6.75 x 8 cm(2)) silicon drift detector with integrated high-voltage divider has been designed, produced and fully characterised in the laboratory by means of ad hoc designed MOS injection electrodes. The detector is of the "butterfly" type, the sensitive area being subdivided into two regions with a maximum drift length of 3.3 cm. The device was also tested in a pion beam (at the CERN PS) tagged by means of a microstrip detector telescope. Bipolar VLSI front-end cells featuring a noise of 250 e(-) rms at 0 pF with a slope of 40 e(-)/pF have been used to read out the signals. The detector showed an excellent stability and featured the expected characteristics. Some preliminary results will be presented. (C) 2000 Elsevier Science B.V. All rights reserved
MH - Italy
MH - Mexico|Distrito Federal
MH - Poland
MH - Russia
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 12
U4 - Instruments & Instrumentation;Nuclear Science & Technology;Physics, Particles & Fields;Spectroscopy
U5 - J;Article
AV - English
IS - 0168-9002
UR - ISI:000084654100034
SO - Nuclear Instruments & Methods in Physics Research Section A-Accelerators Spectrometers Detectors and Associated Equipment 2000 ;439(2-3):476-482
240
UI - 14211
AU - Borboa L
AU - de la Torre C
AD - CSIC, Ctr Invest Biol, E-28006 Madrid, SpainUniv Autonoma Sinaloa, Escuela Med, Culiacan, MexicoBorboa, L, CSIC, Ctr Invest Biol, Velazquez 144, E-28006 Madrid, Spain
TI - Adaptation to Cd(II) and Zn(II), and the caffeine-potentiated override of the G(2) block induced by the checkpoint activated by DNA damage
AB - Moderate and low concentrations of Zn(II) and Cd(II) a ere defined as those which depressed the rate of root elongation in Allium cepa L. to about 40 and 70% respectively of the control (17.3 +/- 4.9 mm/day) at 25 degreesC. At moderate concentrations, cells were detoxified from Cd(II), but not from Zn(II), by inducing the heavy metal chelators phytochelatins. Thus, root elongation further decreased (from 41 to 19% of the control) at moderate (0.05 mM) Cd(II) concentration upon addition of 0.25 mM L-buthionine-[S,R]-sulfoximine (BSO), a specific inhibitor of phytochelatin synthesis. On the other hand, cells were also detoxified from Zn(II) by an alternative mechanism, as the 42% inhibition displayed at 0.5 mM Zn(II) concentration was partially reversed (up to 79%) in the presence of BSO. Zn(II) activated the checkpoint pathway induced by DNA damage, as a transient G(2) block was produced this block was partially cancelled by caffeine, so that chromosomal bridges (but no breaks) were observed in ana-telophase. On the other hand, Cd(II) did not activate the DNA damage checkpoint, as cells entered into anaphase with chromosomal breaks and bridges without any delay Cd(II) may preclude the recognition of DNA damage by altering protein-DNA interactions, since 30% of the metaphases displayed clumped chromosomes. A minimum threshold was required to induce the adaptive responses described here, as BSO did not modify the reduction in root elongation rate recorded at low concentrations of both heavy metals
MH - Mexico|Sinaloa
MH - Spain
PB - SIENA: EDITRICE COMPOSITORI BOLOGNA
RP - NOT IN FILE
U3 - TC 2
U4 - Plant Sciences
U5 - J;Article
AV - English
IS - 1126-3504
UR - ISI:000167095900001
L2 - heavy metals;stress adaptation;DNA damage-dependent checkpoint;caffeine;Allium cepa L.;CELL-CYCLE CHECKPOINTS; METALLOTHIONEIN GENE; CADMIUM; METAL; GENOTOXICITY; EXPRESSION; GROWTH; PLANTS; ZINC; IONS
SO - Plant Biosystems 2000 ;134(1):3-9
241
UI - 15437
AU - Borges-Argaez R
AU - Pena-Rodriguez LM
AU - Waterman PG
AD - So Cross Univ, Ctr Phytochem, Lismore, NSW 2480, AustraliaCtr Invest Cient Yucatan, Grp Quim Organ, Unidad Biotecnol, Merida 97310, Yucatan, MexicoWaterman, PG, So Cross Univ, Ctr Phytochem, POB 157, Lismore, NSW 2480, Australia
TI - Flavonoids from the stem bark of Lonchocarpus xuul
AB - The stem bark of Lonchocarpus xuul (Leguminosae) has yielded four flavonoids which have been identified by spectroscopic methods as the novel 4 beta,5-dimethoxy-6 ",6 "-dimethyl-2H-pyrano-(2 ",3 ":7,6)-flavan (xuulanin), 3 beta,4 beta,5-trimethoxy-6 ",6 "-dimethyl-2H-pyrano-(2 ",3 ":7,6)-flavan (3 beta-methoxyxuulanin), 4 beta-ethoxy-5-methoxy-6 ",6 "-dimethyl-2H-pyrano-(2 ",3 ":7,6)-flavan (4 beta-demethylxuulanin-4 beta-ethyl other), and the known 5,7-dihydroxy-6,8-di(3-methylbut-2-enyl)flavanone (spiniflavanone-B). The ethyl derivative is considered likely to be an artefact. (C) 2000 Elsevier Science Ltd. All rights reserved
MH - Australia
MH - Mexico|Yucatan
PB - OXFORD: PERGAMON-ELSEVIER SCIENCE LTD
RP - NOT IN FILE
U3 - TC 5
U4 - Biochemistry & Molecular Biology;Plant Sciences
U5 - J;Article
AV - English
IS - 0031-9422
UR - ISI:000088715000010
L2 - Lonchocarpus xuul;Leguminosae-Papilionoideae;flavonoids;flavan-4-ol;flavan-3,4-diol;flavanone
SO - Phytochemistry 2000 ;54(6):611-614
242
UI - 16218
AU - Borges G
AU - Walters EE
AU - Kessler RC
AD - Inst Mexicano Psiquiatria, Div Invest Epidemiol & Sociales, Mexico City 14370, DF, MexicoHarvard Univ, Sch Med, Dept Hlth Care Policy, Boston, MA 02115, USABorges, G, Inst Mexicano Psiquiatria, Div Invest Epidemiol & Sociales, Calzada Mexico,Xochimilco 101,Col San Lorenzo, Mexico City 14370, DF, Mexico
TI - Associations of substance use, abuse, and dependence with subsequent suicidal behavior
AB - General population survey data are used to disaggregate the associations of substance use disorders with suicide attempts in order to evaluate a number of hypotheses about the processes leading to these associations. Data are from the US National Comorbidity Survey (1990-1992). Discrete-time survival analysis is used to study the effects of retrospectively reported temporally prior substance use, abuse, and dependence in predicting first onset of suicidal behavior. Alcohol and drug use predict subsequent suicide attempts after controlling for sociodemographics and comorbid mental disorders. Previous use is not a significant predictor among current nonusers. Abuse and dependence are significant predictors among users for three of the 10 substances considered (alcohol, inhalants, and heroin). The number of substances used is more important than the types of substances used in predicting suicidal behavior. Disaggregation shows that the effects of use are largely on suicidal ideation and nonplanned attempts among ideators. In comparison, the effects of use on suicide plans and planned attempts among ideators are not significant. Clinicians need to be aware that current substance use, even in the absence of abuse or dependence, is a significant risk factor for unplanned suicide attempts among ideators
MH - Mexico|Distrito Federal
MH - USA
PB - CARY: OXFORD UNIV PRESS INC
RP - NOT IN FILE
U3 - TC 68
U4 - Public, Environmental & Occupational Health
U5 - J;Article
AV - English
IS - 0002-9262
UR - ISI:000086443700007
L2 - alcohol drinking;comorbidity;mental health;substance-related disorders;suicide;suicide, attempted;NATIONAL-COMORBIDITY-SURVEY; INTERNATIONAL DIAGNOSTIC INTERVIEW; RISK-FACTORS; PSYCHIATRIC-DISORDER; GENERAL-POPULATION; SURVIVAL ANALYSIS; MENTAL-DISORDERS; MARITAL-STATUS; IDEATION; ADOLESCENTS
SO - American Journal of Epidemiology 2000 ;151(8):781-789
243
UI - 14863
AU - Borgonovi F
AU - Izrailev FM
AD - Univ Maryland, Dept Phys, College Pk, MD 20742, USAIst Nazl Fis Mat, Unita Milano, I-22100 Milan, ItalyIst Nazl Fis Nucl, Unita Pavia, I-27100 Pavia, ItalyUniv Autonoma Puebla, Inst Fis, Puebla 72570, MexicoBorgonovi, F, Univ Maryland, Dept Phys, College Pk, MD 20742, USA
TI - Classical statistical mechanics of a few-body interacting spin model
AB - We study the emergence of Boltzmann's law for the ''single-particle energy distribution'' in a closed system of interacting classical spins. It is shown that for a large number of particles Boltzmann's law may occur, even if the interaction is very strong. Specific attention is paid to classical analogs of the average shape of quantum eigenstates and ''local density of states," which are very important in quantum chaology. Analytical predictions are then compared with numerical data
MH - Italy
MH - Mexico|Puebla
MH - USA
PB - COLLEGE PK: AMERICAN PHYSICAL SOC
RP - NOT IN FILE
U3 - TC 6
U4 - Physics, Fluids & Plasmas;Physics, Mathematical
U5 - J;Article
AV - English
IS - 1063-651X
UR - ISI:000165341700081
L2 - FINITE FERMI SYSTEMS; QUANTUM; CHAOS; OSCILLATORS; ERGODICITY; DYNAMICS; NUMBERS; STATES
SO - Physical Review e 2000 ;62(5):6475-6486
244
UI - 14694
AU - Borissova J
AU - Georgiev L
AU - Rosado M
AU - Kurtev R
AU - Bullejos A
AU - Valdez-Gutierrez M
AD - Bulgarian Acad Sci, Inst Astron, BU-1784 Sofia, BulgariaIsaac Newton Inst, Chile Bulgarian Branch, BU-1784 Sofia, BulgariaUniv Nacl Autonoma Mexico, Inst Astron, Mexico City 04510, DF, MexicoUniv Sofia, Dept Astron, Sofia 1164, BulgariaBranch Sofia Univ, Isaac Newton Inst, Sofia 1164, BulgariaInst Nacl Astrofis Opt & Elect, Mexico City, DF, MexicoBorissova, J, Bulgarian Acad Sci, Inst Astron, 72 Tsarigradsko Chaussee, BU-1784 Sofia, Bulgaria
TI - Infrared photometry of the Local Group dwarf irregular galaxy IC 10
AB - We present near infrared JHK photometry for the central area of the irregular dwarf galaxy IC 10. Red stellar population of IC 10 contains young (10-50 Myr) massive red supergiants. Most of AGE stars are younger than 1 Gyr and have masses up to 12 M-.. Comparing the red supergiants of IC 10 and IC 1613 we have determined the reddening of E(B - V) = 1.05 +/- 0.10 and the dereddened distance modulus (m - M)(0) = 23.86 +/- 0.12 mag of Population I stars in IC 10. Detection of six Br gamma emission structures clearly outline two star forming regions in the central area of IC 10. There is no H-2 emission down to 4.65 10(-16) erg(-1)cm(-2) arcsec(-2) indicating that the dominant excitation mechanism of the molecular gas is from UV radiation from hot young stars. From the comparison of Br gamma and H alpha fluxes, we derive average extinction toward the star forming regions E(B - V)H alpha = 1.8 +/- 0 2 The summarized SFR derived from six H alpha and Br gamma emission structures in our field of view is 0.6 M-. year(-1)
MH - Bulgaria
MH - Mexico|Distrito Federal
PB - NEW YORK: SPRINGER-VERLAG
RP - NOT IN FILE
U3 - TC 11
U4 - Astronomy & Astrophysics
U5 - J;Article
AV - English
IS - 0004-6361
UR - ISI:000165873600016
L2 - galaxies : Local Group;galaxies : individual : IC 10;IC 1613;galaxies : stellar content;STELLAR CONTENT; STAR-FORMATION; STANDARD STARS; IC-10; KINEMATICS; DISTANCES; MODELS; COLORS
SO - Astronomy and Astrophysics 2000 ;363(1):130-140
245
UI - 16535
AU - Borowiec AZ
AU - Vazquez-Coutino GA
AD - Univ Wroclaw, Inst Theoret Phys, PL-50204 Wroclaw, PolandUniv Autonoma Metropolitana Iztapalapa, Mexico City 09340, DF, MexicoBorowiec, AZ, Univ Wroclaw, Inst Theoret Phys, Pl Maxa Borna 9, PL-50204 Wroclaw, Poland
TI - Some topics in coalgebra calculus
AB - We study a coderivation from a cobimodule into a coalgebra. Vector cofields are defined by the action of a codual bicomodule on a coalgebra. This action is induced by a codifferential. A construction of a codual object in the category of bicomodules over a given coalgebra has been proposed. Various notions of duality have been analysed in this context
MH - Mexico|Distrito Federal
MH - Poland
PB - PRAGUE: CZECHOSLOVAK JNL OF PHYSICS
RP - NOT IN FILE
U3 - TC 2
U4 - Physics, Multidisciplinary
U5 - J;Article
AV - English
IS - 0011-4626
UR - ISI:000085186700003
SO - Czechoslovak Journal of Physics 2000 ;50(1):23-28
246
UI - 15411
AU - Bottiglieri C
AU - Ferrara L
AU - Corona M
AU - Gurrola GB
AU - Batista C
AU - Wanke E
AU - Possani LD
AD - Natl Autonomous Univ Mexico, Inst Biotechnol, Dept Mol Recognit & Struct Biol, Cuernavaca 62210, Morelos, MexicoCNR, Ctr Int Servizi Spettrometia Massa, IABBAM, I-80147 Naples, ItalyUniv Milan, Biocca, Dept Biotechnol & Biosci, I-20126 Milan, ItalyPossani, LD, Natl Autonomous Univ Mexico, Inst Biotechnol, Dept Mol Recognit & Struct Biol, Avenida Univ 2001,POB 510-3, Cuernavaca 62210, Morelos, Mexico
TI - Disulfide bridges of Ergtoxin, a member of a new sub-family of peptide blockers of the ether-a-go-go-related K+ channel
MH - Italy
MH - Mexico|Morelos
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 2
U4 - Biochemistry & Molecular Biology;Biophysics;Cell Biology
U5 - J;Letter
AV - English
IS - 0014-5793
UR - ISI:000088963900017
L2 - SCORPION
SO - Febs Letters 2000 ;479(3):156-157
247
UI - 16520
AU - Boue M
AU - Dupuis P
AU - Ellis RS
AD - Inst Tecnol Autonomo Mexico, Dept Matemat, Mexico City 01000, DF, MexicoBrown Univ, Div Appl Math, Providence, RI 02912, USAUniv Massachusetts, Dept Math & Stat, Amherst, MA 01003, USABoue, M, Inst Tecnol Autonomo Mexico, Dept Matemat, Rio Hondo 1, Mexico City 01000, DF, Mexico
TI - Large deviations for small noise diffusions with discontinuous statistics
AB - This paper proves the large deviation principle for a class of non-degenerate small noise diffusions with discontinuous drift and with state-dependent diffusion matrix. The proof is based on a variational representation for functionals of strong solutions of stochastic differential equations and on weak convergence methods
MH - Mexico|Distrito Federal
MH - USA
PB - NEW YORK: SPRINGER VERLAG
RP - NOT IN FILE
U3 - TC 4
U4 - Statistics & Probability
U5 - J;Article
AV - English
IS - 0178-8051
UR - ISI:000085268100006
L2 - large deviations;small noise diffusions;discontinuous statistics;SYSTEMS
SO - Probability Theory and Related Fields 2000 ;116(1):125-149
248
UI - 14810
AU - Boulet G
AU - Chehbouni A
AU - Braud I
AU - Vauclin M
AU - Haverkamp R
AU - Zammit C
AD - LTHE CNRS UMR 5564 UJF INPG IRD, F-38041 Grenoble 9, FranceIRD, IMADES, Hermosillo 83190, Sonora, MexicoBoulet, G, CESBIO, 18 Av E Belin,Bpi 2801, F-31401 Toulouse 4, France
TI - A simple water and energy balance model designed for regionalization and remote sensing data utilization
AB - A simple soil-vegetation-atmosphere transfer (SVAT) model designed for scaling applications and remote sensing utilization will be presented. The study is part of the Semi-Arid Land Surface Atmosphere (SALSA) program. The model is built with a single-bucket and single-source representation with a bulk surface of mixed vegetation and soil cover and a single soil reservoir. Classical atmospheric forcing is imposed at a reference level. It uses the concept of infiltration and evaporation capacities to describe water infiltration or exfiltration from a bucket of depth d(r) corresponding to the average infiltration and evaporation depth. The atmospheric forcing is divided into storm and interstorm periods, and both evaporation and infiltration phenomena are described with the well-known three stages representation: one at potential (energy- or rainfall-limited) rate, one at a rate set by the soil water content and one at a zero rate if the water content reaches one of its range limits, namely saturation or residual values. The analytical simplicity of the model is suitable for the investigation of the spatial variability of the mass and energy water balance, and its one-layer representation allows for the direct use of remote sensing data. The model is satisfactorily evaluated using data acquired in the framework of SALSA and a mechanistic complex SVAT model, Simple Soil-Plant-Atmosphere Transfer (SiSPAT) model. (C) 2000 Elsevier Science B.V. All rights reserved
MH - France
MH - Mexico|Sonora
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 16
U4 - Agronomy;Forestry;Meteorology & Atmospheric Sciences
U5 - J;Article
AV - English
IS - 0168-1923
UR - ISI:000165510800009
L2 - SVAT modeling;remote sensing;infiltration and exfiltration capacities;SURFACE-TEMPERATURE; SOIL; VEGETATION; CLIMATE; EVAPOTRANSPIRATION; APPROXIMATION; CALIBRATION; CONDUCTANCE; EVAPORATION; DYNAMICS
SO - Agricultural and Forest Meteorology 2000 ;105(1-3):117-132
249
UI - 14459
AU - Bourges-Waldegg P
AU - Scrivener SAR
AD - Res & Adv Studies Ctr, Mexico City, DF, MexicoCoventry Univ, Coventry, W Midlands, EnglandBourges-Waldegg, P, Ctr Invest & Estudios Avanzados, Rincon Colonial Calacoaya, Atizapan 53996, Mexico
TI - Applying and testing an approach to design for culturally diverse user groups
AB - This paper intends to illustrate how user interface designers can apply the Meaning in Mediated Action (MIMA) approach (P. Bourges-Waldegg. A.R. Scrivener, Meaning; the central issue is crosscultural HCI design, Interacting with Computers, 9 (3) (1998) 287-310, special issue on "Shared Values and Shared Interfaces") to design for culturally diverse user groups. After outlining its theoretical foundation, we describe how the MIMA stages-observation, evaluation, analysis and design-were carried out to redesign a WWW system. Finally, we assess the efficacy of this approach by comparing the results of the evaluation of the original and the redesigned interfaces. (C) 2000 Elsevier Science B.V. All rights reserved
MH - United Kingdom
MH - Mexico|Estado De Mexico
MH - Mexico|Distrito Federal
PB - AMSTERDAM: ELSEVIER SCIENCE BV
RP - NOT IN FILE
U3 - TC 2
U4 - Computer Science, Cybernetics;Ergonomics
U5 - J;Article
AV - English
IS - 0953-5438
UR - ISI:000166449500001
L2 - culture;interface design;representation;meaning;context
SO - Interacting with Computers 2000 ;13(2):111-126
250
UI - 16201
AU - Bourgois J
AU - Guivel C
AU - Lagabrielle Y
AU - Calmus T
AU - Boulegue J
AU - Daux V
AD - Univ Paris 06, CNRS, Lab Geodynam Tecton & Environm, F-75252 Paris 05, FranceUniv Paris 06, Lab Geochim & Met Gen, F-75252 Paris, FranceUniv Autonoma Mexico, Inst Geol, Hermosillo, Sonora, MexicoUniv Paris 06, Lab Geol Sedimentaire, F-75252 Paris 05, FranceUniv Nantes, Lab Planetol & Geodynam, F-44322 Nantes 3, FranceInst Rech Dev, Noumea, New CaledoniaBourgois, J, Univ Paris 06, CNRS, Lab Geodynam Tecton & Environm, Tour 16-26,4eme Etage,Boite 119,4 Pl Jussieu, F-75252 Paris 05, France
TI - Glacial-interglacial trench supply variation, spreading-ridge subduction, and feedback controls on the Andean margin development at the Chile triple junction area (45-48 degrees S)
AB - During the Chile triple junction (CTJ) cruise (March-April 1997), EM12 bathymetry and seismic reflection data were collected in the vicinity of the Chile triple junction (45-48 degrees S), where an active spreading ridge is being subducted beneath the Andean continental margin. Results show a continental margin development shaped by tectonic processes spanning a spectrum from subduction-erosion to subduction-accretion. The Andean continental margin and the Chile trench exhibit a strong segmentation which reflects the slab segmentation and the Chile triple junction migration. Three segments were identified along the Andean continental margin: the presubduction, the synsubduction, and the postsubduction segments, from north to south. Both climate-induced variations of the sediment supply to the trench and the tectonic reorganization at the Nazca-Antarctica plate boundary involving postsubduction ridge jump are the two main factors that control the tectonic regime of this continental margin. Along the survey area we infer the succession of two different periods during the last glacial-interglacial cycle: a glacial period with ice-rafted detrital discharges restricted to the shoreline area and low river output and a warmer period during which the Andean ice cap retreat allowed the Andes to be drained off. During these warm periods, rapid increase in trench deposition caused the margin to switch from subduction-erosion or nonaccretion to subduction-accretion: (1) along the presubduction segment after the last deglaciation and (2) along the postsubduction segment after the interglacial episode at 130-117 ka. Conversely, a nonaccretion or subduction-erosion mode characterized the presubduction and postsubduction segments during glacial maximums. The major effects of subduction of the buoyant Chile ridge include a shallow trench which diverts trench sediment supply and tectonic instabilities at the Nazca-Antarctica plate boundary. We suggest that a postsubduction westward jump of the Chile ridge occurred during the past 780 kyr. It produced slab fragmentation and individualization of an ephemeral microplate north of the 'Taitao fracture zone: the Chonos microplate. In 780 kyr, two episodes of subduction-accretion separated by an episode of subduction-erosion occurred in relation with the Chonos microplate individualization and subduction. The current northward migration of the triple junction along the Chonos microplate-South America plate boundary introduces a sharp change in the tectonic mode from subduction-erosion to the north to subduction-accretion to the south. The data collected along the Taitao ridge have revealed the complex three-dimensional structure of an accretionary wedge which includes a midslope thrust sheet exhibiting the characteristics of an ophiolite: the Taitao Ridge ophiolite. No connection exists between the Taitao Ridge ophiolite and the Bahia Barrientos ophiolite cropping out onland in the Taitao peninsula
MH - France
MH - Mexico|Sonora
MH - New Caledonia
PB - WASHINGTON: AMER GEOPHYSICAL UNION
RP - NOT IN FILE
U3 - TC 13
U4 - Geochemistry & Geophysics
U5 - J;Article
AV - English
IS - 0148-0227
UR - ISI:000086437500033
L2 - SOUTHERN CHILE; TECTONIC EROSION; CONVERGENT MARGINS; PLATE; COLLISION; AMERICA; ZONE; MANIFESTATIONS; CONSEQUENCES; GEOCHEMISTRY
SO - Journal of Geophysical Research-Solid Earth 2000 ;105(B4):8355-8386
251
UI - 14606
AU - Bousquet J
AU - D'Urzo A
AU - Hebert J
AU - Barraza CH
AU - Boulet LP
AU - Suarez-Chacon R
AU - Harnest U
AU - Lundback B
AU - Morales GM
AU - Nieminen MM
AU - Nolop KB
AU - Visser S
AU - Lutsky BN
AD - Hop Arnaud de Villeneuve, Serv Malad Resp, F-34059 Montpellier, FrancePrimary Care Asthma Clin, Toronto, ON, CanadaHosp Clin Parque, Chihuahua, MexicoHop Laval, Quebec City, PQ, CanadaPoliclin Metropolitana, Caracas, VenezuelaBodens Sjukhus, Dept Med, Boden, SwedenHosp Gen Enfermedad Comun, IGSS, Guatemala, CA, USATampere Univ Hosp, Tampere, FinlandSchering Plough Res Inst, Kenilworth, NJ, USAHF Verwoerd Hosp, Dept Internal Med, Pretoria, South AfricaBousquet, J, Hop Arnaud de Villeneuve, Serv Malad Resp, 555 Route Ganges, F-34059 Montpellier, France
TI - Comparison of the efficacy and safety of mometasone furoate dry powder inhaler to budesonide Turbuhaler (R)
AB - Mometasone furoate (MF) administered by dry powder inhaler (DPI) was composed with budesonide (BUD) Turbuhaler(R) in the treatment of moderate persistent asthma. The patients were randomized to one of four treatment groups: MF DPI (100, 200, 400 mug b.i.d) or BUD Turbuhaler(R). 400 mug b.i.d in a 12-week, active-controlled, evaluator-blind, multicentre international trial. The primary efficacy variable was the mean change from baseline to endpoint Oast treatment visit) in forced expiratory volume in one second (FEV1), Changes in FEV1 showed a statistically significant superiority (p<0.05) of MF DPI 200 and 400 ) of mixed fee CoNPdM and CoNRhM (N, M = 19, 24) clusters are determined by using a self-consistent real-space tight binding method. In all cases considered,