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25 April 2024
 
  » pubmed » pmid15190311

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A precision measurement of the mass of the top quark
V M Abazov ; B Abbott ; A Abdesselam ; M Abolins ; V Abramov ; B S Acharya ; D L Adams ; M Adams ; S N Ahmed ; G D Alexeev ; A Alton ; G A Alves ; Y Arnoud ; C Avila ; V V Babintsev ; L Babukhadia ; T C Bacon ; A Baden ; S Baffioni ; B Baldin ; P W Balm ; S Banerjee ; E Barberis ; P Baringer ; J Barreto ; J F Bartlett ; U Bassler ; D Bauer ; A Bean ; F Beaudette ; M Begel ; A Belyaev ; S B Beri ; G Bernardi ; I Bertram ; A Besson ; R Beuselinck ; V A Bezzubov ; P C Bhat ; V Bhatnagar ; M Bhattacharjee ; G Blazey ; F Blekman ; S Blessing ; A Boehnlein ; N I Bojko ; T A Bolton ; F Borcherding ; K Bos ; T Bose ; A Brandt ; G Briskin ; R Brock ; G Brooijmans ; A Bross ; D Buchholz ; M Buehler ; V Buescher ; V S Burtovoi ; J M Butler ; F Canelli ; W Carvalho ; D Casey ; H Castilla-Valdez ; D Chakraborty ; K M Chan ; S V Chekulaev ; D K Cho ; S Choi ; S Chopra ; D Claes ; A R Clark ; B Connolly ; W E Cooper ; D Coppage ; S Crépé-Renaudin ; M A C Cummings ; D Cutts ; H Da Motta ; G A Davis ; K De ; S J De Jong ; M Demarteau ; R Demina ; P Demine ; D Denisov ; S P Denisov ; S Desai ; H T Diehl ; M Diesburg ; S Doulas ; L V Dudko ; L Duflot ; S R Dugad ; A Duperrin ; A Dyshkant ; D Edmunds ; J Ellison ; J T Eltzroth ; V D Elvira ; R Engelmann ; S Eno ; G Eppley ; P Ermolov ; O V Eroshin ; J Estrada ; H Evans ; V N Evdokimov ; T Ferbel ; F Filthaut ; H E Fisk ; M Fortner ; H Fox ; S Fu ; S Fuess ; E Gallas ; A N Galyaev ; M Gao ; V Gavrilov ; R J Genik ; K Genser ; C E Gerber ; Y Gershtein ; G Ginther ; B Gómez ; P I Goncharov ; K Gounder ; A Goussiou ; P D Grannis ; H Greenlee ; Z D Greenwood ; S Grinstein ; L Groer ; S Grünendahl ; M W Grünewald ; S N Gurzhiev ; G Gutierrez ; P Gutierrez ; N J Hadley ; H Haggerty ; S Hagopian ; V Hagopian ; R E Hall ; C Han ; S Hansen ; J M Hauptman ; C Hebert ; D Hedin ; J M Heinmiller ; A P Heinson ; U Heintz ; M D Hildreth ; R Hirosky ; J D Hobbs ; B Hoeneisen ; J Huang ; Y Huang ; I Iashvili ; R Illingworth ; A S Ito ; M Jaffré ; S Jain ; R Jesik ; K Johns ; M Johnson ; A Jonckheere ; H Jöstlein ; A Juste ; W Kahl ; S Kahn ; E Kajfasz ; A M Kalinin ; D Karmanov ; D Karmgard ; R Kehoe ; S Kesisoglou ; A Khanov ; A Kharchilava ; B Klima ; J M Kohli ; A V Kostritskiy ; J Kotcher ; B Kothari ; A V Kozelov ; E A Kozlovsky ; J Krane ; M R Krishnaswamy ; P Krivkova ; S Krzywdzinski ; M Kubantsev ; S Kuleshov ; Y Kulik ; S Kunori ; A Kupco ; V E Kuznetsov ; G Landsberg ; W M Lee ; A Leflat ; F Lehner ; C Leonidopoulos ; J Li ; Q Z Li ; J G R Lima ; D Lincoln ; S L Linn ; J Linnemann ; R Lipton ; A Lucotte ; L Lueking ; C Lundstedt ; C Luo ; A K A Maciel ; R J Madaras ; V L Malyshev ; V Manankov ; H S Mao ; T Marshall ; M I Martin ; S E K Mattingly ; A A Mayorov ; R McCarthy ; T McMahon ; H L Melanson ; A Melnitchouk ; A Merkin ; K W Merritt ; C Miao ; H Miettinen ; D Mihalcea ; N Mokhov ; N K Mondal ; H E Montgomery ; R W Moore ; Y D Mutaf ; E Nagy ; M Narain ; V S Narasimham ; N A Naumann ; H A Neal ; J P Negret ; S Nelson ; A Nomerotski ; T Nunnemann ; D O’Neil ; V Oguri ; N Oshima ; P Padley ; K Papageorgiou ; N Parashar ; R Partridge ; N Parua ; A Patwa ; O Peters ; P Pétroff ; R Piegaia ; B G Pope ; H B Prosper ; S Protopopescu ; M B Przybycien ; J Qian ; S Rajagopalan ; P A Rapidis ; N W Reay ; S Reucroft ; M Ridel ; M Rijssenbeek ; F Rizatdinova ; T Rockwell ; C Royon ; P Rubinov ; R Ruchti ; B M Sabirov ; G Sajot ; A Santoro ; L Sawyer ; R D Schamberger ; H Schellman ; A Schwartzman ; E Shabalina ; R K Shivpuri ; D Shpakov ; M Shupe ; R A Sidwell ; V Simak ; V Sirotenko ; P Slattery ; R P Smith ; G R Snow ; J Snow ; S Snyder ; J Solomon ; Y Song ; V Sorín ; M Sosebee ; N Sotnikova ; K Soustruznik ; M Souza ; N R Stanton ; G Steinbrück ; D Stoker ; V Stolin ; A Stone ; D A Stoyanova ; M A Strang ; M Strauss ; M Strovink ; L Stutte ; A Sznajder ; M Talby ; W Taylor ; S Tentindo-Repond ; T G Trippe ; A S Turcot ; P M Tuts ; R Van Kooten ; V Vaniev ; N Varelas ; F Villeneuve-Seguier ; A A Volkov ; A P Vorobiev ; H D Wahl ; Z-M Wang ; J Warchol ; G Watts ; M Wayne ; H Weerts ; A White ; D Whiteson ; D A Wijngaarden ; S Willis ; S J Wimpenny ; J Womersley ; D R Wood ; Q Xu ; R Yamada ; T Yasuda ; Y A Yatsunenko ; K Yip ; J Yu ; M Zanabria ; X Zhang ; B Zhou ; Z Zhou ; M Zielinski ; D Zieminska ; A Zieminski ; V Zutshi ; E G Zverev ; A Zylberstejn ; ;
Date 10 Jun 2004
Journal Nature, 429 (6992), 638-42
AbstractThe standard model of particle physics contains parameters--such as particle masses--whose origins are still unknown and which cannot be predicted, but whose values are constrained through their interactions. In particular, the masses of the top quark (M(t)) and W boson (M(W)) constrain the mass of the long-hypothesized, but thus far not observed, Higgs boson. A precise measurement of M(t) can therefore indicate where to look for the Higgs, and indeed whether the hypothesis of a standard model Higgs is consistent with experimental data. As top quarks are produced in pairs and decay in only about 10(-24) s into various final states, reconstructing their masses from their decay products is very challenging. Here we report a technique that extracts more information from each top-quark event and yields a greatly improved precision (of +/- 5.3 GeV/c2) when compared to previous measurements. When our new result is combined with our published measurement in a complementary decay mode and with the only other measurements available, the new world average for M(t) becomes 178.0 +/- 4.3 GeV/c2. As a result, the most likely Higgs mass increases from the experimentally excluded value of 96 to 117 GeV/c2, which is beyond current experimental sensitivity. The upper limit on the Higgs mass at the 95% confidence level is raised from 219 to 251 GeV/c2.
Source PubMed, pmid15190311 doi: 10.1038/nature02589
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