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Measurement of the top quark pair production cross section in pp̄ collisions using multijet final states
Authors
B Abbott
M Abolins
+363 more
V Abramov
BS Acharya
I Adam
DL Adams
M Adams
S Ahn
H Aihara
GA Alves
N Amos
EW Anderson
MM Baarmand
VV Babintsev
L Babukhadia
A Baden
B Baldin
S Banerjee
J Bantly
E Barberis
P Baringer
JF Bartlett
A Belyaev
SB Beri
I Bertram
VA Bezzubov
PC Bhat
V Bhatnagar
M Bhattacharjee
N Biswas
G Blazey
S Blessing
P Bloom
A Boehnlein
NI Bojko
F Borcherding
C Boswell
A Brandt
R Breedon
R Brock
A Bross
D Buchholz
VS Burtovoi
JM Butler
W Carvalho
D Casey
Z Casilum
H Castilla-Valdez
D Chakraborty
S-M Chang
SV Chekulaev
W Chen
S Choi
S Chopra
BC Choudhary
JH Christenson
M Chung
D Claes
AR Clark
WG Cobau
J Cochran
L Coney
WE Cooper
C Cretsinger
D Cullen-Vidal
MAC Cummings
D Cutts
H Da Motta
OI Dahl
K Davis
K De
K Del Signore
M Demarteau
D Denisov
SP Denisov
G Di Loreto
HT Diehl
M Diesburg
P Draper
Y Ducros
LV Dudko
SR Dugad
A Dyshkant
D Edmunds
J Ellison
VD Elvira
R Engelmann
S Eno
G Eppley
P Ermolov
OV Eroshin
VN Evdokimov
T Fahland
MK Fatyga
S Feher
D Fein
T Ferbel
G Finocchiaro
HE Fisk
Y Fisyak
E Flattum
GE Forden
M Fortner
KC Frame
S Fuess
E Gallas
AN Galyaev
P Gartung
V Gavrilov
TL Geld
RJ Genik II
K Genser
CE Gerber
Y Gershtein
B Gibbard
B Gobbi
PI Goncharov
JL González Solís
H Gordon
LT Goss
K Gounder
A Goussiou
N Graf
PD Grannis
DR Green
H Greenlee
S Grinstein
P Grudberg
S Grünendahl
G Guglielmo
JA Guida
JM Guida
A Gupta
SN Gurzhiev
G Gutierrez
P Gutierrez
B Gómez
G Gómez
NJ Hadley
H Haggerty
S Hagopian
V Hagopian
KS Hahn
RE Hall
P Hanlet
S Hansen
JM Hauptman
D Hedin
AP Heinson
U Heintz
R Hernández-Monloya
T Heuring
R Hirosky
JD Hobbs
B Hoeneisen
JS Hoftun
F Hsieh
T Hu
AS Ito
J Jaques
SA Jerger
R Jesik
T Joffe-Minor
K Johns
M Johnson
A Jonckheere
M Jones
SY Jun
CK Jung
H Jöstlein
S Kahn
G Kalbfleisch
D Karmanov
D Karmgard
R Kehoe
ML Kelly
SK Kim
B Klima
C Klopfenstein
W Ko
JM Kohli
D Koltick
AV Kostritskiy
J Kotcher
AV Kotwal
AV Kozelov
EA Kozlovsky
J Krane
MR Krishnaswamy
S Krzywdzinski
S Kuleshov
Y Kulik
S Kunori
F Landry
G Landsberg
B Lauer
A Leflat
J Li
QZ Li
JGR Lima
D Lincoln
SL Linn
J Linnemann
R Lipton
F Lobkowicz
SC Loken
A Lucotte
L Lueking
AL Lyon
AKA Maciel
RJ Madaras
R Madden
L Magaña-Mendoza
V Manankov
S Mani
HS Mao
R Markeloff
T Marshall
MI Martin
KM Mauritz
B May
AA Mayorov
R McCarthy
J McDonald
T McKibben
J McKinley
T McMahon
HL Melanson
M Merkin
KW Merritt
C Miao
H Miettinen
A Mincer
CS Mishra
N Mokhov
NK Mondal
HE Montgomery
P Mooney
J Moromisato
M Mostafa
C Murphy
F Nang
M Narain
VS Narasimham
A Narayanan
HA Neal
JP Negret
P Nemethy
D Norman
L Oesch
V Oguri
E Oliveira
E Oltman
N Oshima
D Owen
P Padley
A Para
YM Park
R Partridge
N Parua
M Paterno
B Pawlik
J Perkins
M Peters
R Piegaia
H Piekarz
Y Pischalnikov
BG Pope
HB Prosper
S Protopopescu
J Qian
PZ Quintas
R Raja
S Rajagopalan
O Ramirez
S Reucroft
M Rijssenbeek
T Rockwell
M Roco
P Rubinov
R Ruchti
J Rutherfoord
A Santoro
L Sawyer
RD Schamberger
H Schellman
J Sculli
E Shabalina
C Shaffer
HC Shankar
RK Shivpuri
D Shpakov
M Shupe
H Singh
JB Singh
V Sirotenko
E Smith
RP Smith
R Snihur
GR Snow
J Snow
S Snyder
J Solomon
M Sosebee
N Sotnikova
M Souza
G Steinbrück
RW Stephens
ML Stevenson
F Stichelbaut
D Stoker
V Stolin
DA Stoyanova
M Strauss
K Streets
M Strovink
A Sznajder
A Sánchez-Hernández
P Tamburello
J Tarazi
M Tartaglia
TLT Thomas
J Thompson
TG Trippe
PM Tuts
V Vaniev
N Varelas
EW Varnes
D Vititoe
AA Volkov
AP Vorobiev
HD Wahl
G Wang
J Warchol
G Watts
M Wayne
H Weerts
A White
JT White
JA Wightman
S Willis
SJ Wimpenny
JVD Wirjawan
J Womersley
E Won
DR Wood
Z Wu
R Yamada
P Yamin
T Yasuda
P Yepes
K Yip
C Yoshikawa
S Youssef
J Yu
Y Yu
B Zhang
Y Zhou
Z Zhou
ZH Zhu
M Zielinski
D Zieminska
A Zieminski
EG Zverev
A Zylberstejn
Publication date
1 January 1999
Publisher
Abstract
We have studied tt̄ production using multijet final states in pp̄ collisions at a center-of-mass energy of 1.8 TeV, with an integrated luminosity of 110.3 pb-1. Each of the top quarks with these final states decays exclusively to a bottom quark and a W boson, with the W bosons decaying into quark-antiquark pairs. The analysis has been optimized using neural networks to achieve the smallest expected fractional uncertainty on the tt̄ production cross section, and yields a cross section of 7.1±2.8 (stat)±1.5 (syst) pb, assuming a top quark mass of 172.1 GeV/c2. Combining this result with previous DØ measurements, where one or both of the W bosons decay leptonically, gives a tt̄ production cross section of 5.9±1.2 (stat)±1.1 (syst) pb. ©1999 The American Physical Society
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Last time updated on 30/09/2015
Oxford University Research Archive (ORA)
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Last time updated on 18/04/2020