Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV

This paper describes a measurement of the top quark mass, Mtop, with the dynamical likelihood method (DLM) using the CDF II detector at the Fermilab Tevatron. The Tevatron produces top/antitop (tt̄) pairs in pp̄ collisions at a center-of-mass energy of 1.96 TeV. The data sample used in this analysis...

Full description

Bibliographic Details
Main Authors: Abulencia, A, Acosta, D, Adelman, J, Affolder, T, Akimoto, T, Albrow, MG, Ambrose, D, Amerio, S, Amidei, D, Anastassov, A, Anikeev, K, Annovi, A, Antos, J, Aoki, M, Apollinari, G, Arguin, J, Arisawa, T, Artikov, A, Ashmanskas, W, Attal, A, Azfar, F, Azzi-Bacchetta, P, Azzurri, P, Bacchetta, N, Bachacou, H
Format: Journal article
Language:English
Published: 2006
_version_ 1826263481479856128
author Abulencia, A
Acosta, D
Adelman, J
Affolder, T
Akimoto, T
Albrow, MG
Ambrose, D
Amerio, S
Amidei, D
Anastassov, A
Anikeev, K
Annovi, A
Antos, J
Aoki, M
Apollinari, G
Arguin, J
Arisawa, T
Artikov, A
Ashmanskas, W
Attal, A
Azfar, F
Azzi-Bacchetta, P
Azzurri, P
Bacchetta, N
Bachacou, H
author_facet Abulencia, A
Acosta, D
Adelman, J
Affolder, T
Akimoto, T
Albrow, MG
Ambrose, D
Amerio, S
Amidei, D
Anastassov, A
Anikeev, K
Annovi, A
Antos, J
Aoki, M
Apollinari, G
Arguin, J
Arisawa, T
Artikov, A
Ashmanskas, W
Attal, A
Azfar, F
Azzi-Bacchetta, P
Azzurri, P
Bacchetta, N
Bachacou, H
author_sort Abulencia, A
collection OXFORD
description This paper describes a measurement of the top quark mass, Mtop, with the dynamical likelihood method (DLM) using the CDF II detector at the Fermilab Tevatron. The Tevatron produces top/antitop (tt̄) pairs in pp̄ collisions at a center-of-mass energy of 1.96 TeV. The data sample used in this analysis was accumulated from March 2002 through August 2004, which corresponds to an integrated luminosity of 318pb-1. We use the tt̄ candidates in the "lepton+jets" decay channel, requiring at least one jet identified as a b quark by finding a displaced secondary vertex. The DLM defines a likelihood for each event based on the differential cross section as a function of Mtop per unit phase space volume of the final partons, multiplied by the transfer functions from jet to parton energies. The method takes into account all possible jet combinations in an event, and the likelihood is multiplied event by event to derive the top quark mass by the maximum likelihood method. Using 63 tt̄ candidates observed in the data, with 9.2 events expected from background, we measure the top quark mass to be 173.2+2.6-2.4(stat.)±3. 2(syst.)GeV/c2, or 173.2+4.1-4.0GeV/c2. © 2006 The American Physical Society.
first_indexed 2024-03-06T19:52:27Z
format Journal article
id oxford-uuid:24692e47-e5e5-4999-9ce7-c059208b82ff
institution University of Oxford
language English
last_indexed 2024-03-06T19:52:27Z
publishDate 2006
record_format dspace
spelling oxford-uuid:24692e47-e5e5-4999-9ce7-c059208b82ff2022-03-26T11:50:03ZMeasurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeVJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:24692e47-e5e5-4999-9ce7-c059208b82ffEnglishSymplectic Elements at Oxford2006Abulencia, AAcosta, DAdelman, JAffolder, TAkimoto, TAlbrow, MGAmbrose, DAmerio, SAmidei, DAnastassov, AAnikeev, KAnnovi, AAntos, JAoki, MApollinari, GArguin, JArisawa, TArtikov, AAshmanskas, WAttal, AAzfar, FAzzi-Bacchetta, PAzzurri, PBacchetta, NBachacou, HThis paper describes a measurement of the top quark mass, Mtop, with the dynamical likelihood method (DLM) using the CDF II detector at the Fermilab Tevatron. The Tevatron produces top/antitop (tt̄) pairs in pp̄ collisions at a center-of-mass energy of 1.96 TeV. The data sample used in this analysis was accumulated from March 2002 through August 2004, which corresponds to an integrated luminosity of 318pb-1. We use the tt̄ candidates in the "lepton+jets" decay channel, requiring at least one jet identified as a b quark by finding a displaced secondary vertex. The DLM defines a likelihood for each event based on the differential cross section as a function of Mtop per unit phase space volume of the final partons, multiplied by the transfer functions from jet to parton energies. The method takes into account all possible jet combinations in an event, and the likelihood is multiplied event by event to derive the top quark mass by the maximum likelihood method. Using 63 tt̄ candidates observed in the data, with 9.2 events expected from background, we measure the top quark mass to be 173.2+2.6-2.4(stat.)±3. 2(syst.)GeV/c2, or 173.2+4.1-4.0GeV/c2. © 2006 The American Physical Society.
spellingShingle Abulencia, A
Acosta, D
Adelman, J
Affolder, T
Akimoto, T
Albrow, MG
Ambrose, D
Amerio, S
Amidei, D
Anastassov, A
Anikeev, K
Annovi, A
Antos, J
Aoki, M
Apollinari, G
Arguin, J
Arisawa, T
Artikov, A
Ashmanskas, W
Attal, A
Azfar, F
Azzi-Bacchetta, P
Azzurri, P
Bacchetta, N
Bachacou, H
Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV
title Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV
title_full Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV
title_fullStr Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV
title_full_unstemmed Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV
title_short Measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b-tags in pp̄ collisions at s=1.96TeV
title_sort measurement of the top quark mass with the dynamical likelihood method using lepton plus jets events with b tags in pp collisions at s 1 96tev
work_keys_str_mv AT abulenciaa measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT acostad measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT adelmanj measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT affoldert measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT akimotot measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT albrowmg measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT ambrosed measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT amerios measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT amideid measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT anastassova measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT anikeevk measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT annovia measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT antosj measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT aokim measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT apollinarig measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT arguinj measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT arisawat measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT artikova measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT ashmanskasw measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT attala measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT azfarf measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT azzibacchettap measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT azzurrip measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT bacchettan measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev
AT bachacouh measurementofthetopquarkmasswiththedynamicallikelihoodmethodusingleptonplusjetseventswithbtagsinppcollisionsats196tev