Direct measurement of the top quark mass
We measure the top quark mass mt using tt̄ pairs produced in the D0 detector by √s = 1.8 TeV pp̄ collisions in a 125 pb-1 exposure at the Fermilab Tevatron. We make a two constraint fit to mt in tt̄ → bW+b̄W- final states with one W decaying to qq̄ and the other to eν or μν. Events are binned in fit...
Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , , |
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Format: | Journal article |
Language: | English |
Published: |
1997
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author | Abachi, S Abbott, B Abolins, M Acharya, B Adam, I Adams, D Adams, M Ahn, S Aihara, H Alves, G Amidi, E Amos, N Anderson, E Astur, R Baarmand, M Baden, A Balamurali, V Balderston, J Baldin, B Banerjee, S Bantly, J Barberis, E Bartlett, J Bazizi, K Belyaev, A |
author_facet | Abachi, S Abbott, B Abolins, M Acharya, B Adam, I Adams, D Adams, M Ahn, S Aihara, H Alves, G Amidi, E Amos, N Anderson, E Astur, R Baarmand, M Baden, A Balamurali, V Balderston, J Baldin, B Banerjee, S Bantly, J Barberis, E Bartlett, J Bazizi, K Belyaev, A |
author_sort | Abachi, S |
collection | OXFORD |
description | We measure the top quark mass mt using tt̄ pairs produced in the D0 detector by √s = 1.8 TeV pp̄ collisions in a 125 pb-1 exposure at the Fermilab Tevatron. We make a two constraint fit to mt in tt̄ → bW+b̄W- final states with one W decaying to qq̄ and the other to eν or μν. Events are binned in fit mass versus a measure of probability for events to be signal rather than background. Likelihood fits to the data yield mt = 173.3 ± 5.6(stat) ± 6.2(syst) GeV/c2. |
first_indexed | 2024-03-07T02:50:08Z |
format | Journal article |
id | oxford-uuid:ad6688ec-12cc-48ef-8594-1cf8e38afdba |
institution | University of Oxford |
language | English |
last_indexed | 2024-03-07T02:50:08Z |
publishDate | 1997 |
record_format | dspace |
spelling | oxford-uuid:ad6688ec-12cc-48ef-8594-1cf8e38afdba2022-03-27T03:35:23ZDirect measurement of the top quark massJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:ad6688ec-12cc-48ef-8594-1cf8e38afdbaEnglishSymplectic Elements at Oxford1997Abachi, SAbbott, BAbolins, MAcharya, BAdam, IAdams, DAdams, MAhn, SAihara, HAlves, GAmidi, EAmos, NAnderson, EAstur, RBaarmand, MBaden, ABalamurali, VBalderston, JBaldin, BBanerjee, SBantly, JBarberis, EBartlett, JBazizi, KBelyaev, AWe measure the top quark mass mt using tt̄ pairs produced in the D0 detector by √s = 1.8 TeV pp̄ collisions in a 125 pb-1 exposure at the Fermilab Tevatron. We make a two constraint fit to mt in tt̄ → bW+b̄W- final states with one W decaying to qq̄ and the other to eν or μν. Events are binned in fit mass versus a measure of probability for events to be signal rather than background. Likelihood fits to the data yield mt = 173.3 ± 5.6(stat) ± 6.2(syst) GeV/c2. |
spellingShingle | Abachi, S Abbott, B Abolins, M Acharya, B Adam, I Adams, D Adams, M Ahn, S Aihara, H Alves, G Amidi, E Amos, N Anderson, E Astur, R Baarmand, M Baden, A Balamurali, V Balderston, J Baldin, B Banerjee, S Bantly, J Barberis, E Bartlett, J Bazizi, K Belyaev, A Direct measurement of the top quark mass |
title | Direct measurement of the top quark mass |
title_full | Direct measurement of the top quark mass |
title_fullStr | Direct measurement of the top quark mass |
title_full_unstemmed | Direct measurement of the top quark mass |
title_short | Direct measurement of the top quark mass |
title_sort | direct measurement of the top quark mass |
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