Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector
A measurement of the mass difference between top and anti-top quarks is presented. In a 4.7 fb −1 data sample of proton–proton collisions at s=7 TeV recorded with the ATLAS detector at the LHC, events consistent with tt¯ production and decay into a single charged lepton final state are reconstructed...
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todo:paper_03702693_v728_n_p363_Aad2023-10-03T15:29:34Z Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector Aad, G. A measurement of the mass difference between top and anti-top quarks is presented. In a 4.7 fb −1 data sample of proton–proton collisions at s=7 TeV recorded with the ATLAS detector at the LHC, events consistent with tt¯ production and decay into a single charged lepton final state are reconstructed. For each event, the mass difference between the top and anti-top quark candidate is calculated. A two b-tag requirement is used in order to reduce the background contribution. A maximum likelihood fit to these per-event mass differences yields Δm≡m t −m t¯ =0.67±0.61(stat)±0.41(syst) GeV, consistent with CPT invariance. © 2013 The Authors JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_03702693_v728_n_p363_Aad |
institution |
Universidad de Buenos Aires |
institution_str |
I-28 |
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R-134 |
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Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) |
description |
A measurement of the mass difference between top and anti-top quarks is presented. In a 4.7 fb −1 data sample of proton–proton collisions at s=7 TeV recorded with the ATLAS detector at the LHC, events consistent with tt¯ production and decay into a single charged lepton final state are reconstructed. For each event, the mass difference between the top and anti-top quark candidate is calculated. A two b-tag requirement is used in order to reduce the background contribution. A maximum likelihood fit to these per-event mass differences yields Δm≡m t −m t¯ =0.67±0.61(stat)±0.41(syst) GeV, consistent with CPT invariance. © 2013 The Authors |
format |
JOUR |
author |
Aad, G. |
spellingShingle |
Aad, G. Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector |
author_facet |
Aad, G. |
author_sort |
Aad, G. |
title |
Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector |
title_short |
Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector |
title_full |
Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector |
title_fullStr |
Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector |
title_full_unstemmed |
Measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 TeV using the ATLAS detector |
title_sort |
measurement of the mass difference between top and anti-top quarks in pp collisions at √s=7 tev using the atlas detector |
url |
http://hdl.handle.net/20.500.12110/paper_03702693_v728_n_p363_Aad |
work_keys_str_mv |
AT aadg measurementofthemassdifferencebetweentopandantitopquarksinppcollisionsats7tevusingtheatlasdetector |
_version_ |
1807320911605399552 |