Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV

The ratio of the top-quark branching fractions R=B(t→Wb)/B(t→Wq), where the denominator includes the sum over all down-type quarks (q=b,s,d), is measured in the t[¯ overt] dilepton final state with proton–proton collision data at √s=8 TeV from an integrated luminosity of 19.7 fb[superscript −1], col...

Full description

Bibliographic Details
Main Authors: Apyan, Aram, Barbieri, Richard Alexander, Bauer, Gerry P, Busza, Wit, Cali, Ivan Amos, Di Matteo, Leonardo, Dutta, Valentina, Gomez-Ceballos, Guillelmo, Goncharov, Maxim, Gulhan, Doga Can, Klute, Markus, Lai, Yue Shi, Lee, Yen-Jie, Levin, Andrew Michael, Luckey Jr, P David, Ma, Teng, Paus, Christoph M. E., Ralph, Duncan Kelley, Roland, Christof E, Roland, Gunther M, Stephans, George S. F., Stoeckli, Fabian, Sumorok, Konstanty C, Velicanu, Dragos Alexandru, Veverka, Jan, Wyslouch, Boleslaw, Yang, Mingming, Zanetti, Marco, Wyslouch, Victoria, Chan, M.
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Published: Elsevier BV 2018
Online Access:http://hdl.handle.net/1721.1/117038
https://orcid.org/0000-0002-9418-6656
https://orcid.org/0000-0002-7945-005X
https://orcid.org/0000-0002-3831-9071
https://orcid.org/0000-0002-2822-3375
https://orcid.org/0000-0001-9236-6621
https://orcid.org/0000-0002-0869-5631
https://orcid.org/0000-0003-1486-606X
https://orcid.org/0000-0003-2593-7767
https://orcid.org/0000-0002-1136-6900
https://orcid.org/0000-0002-6047-4211
https://orcid.org/0000-0001-8983-2169
https://orcid.org/0000-0003-3106-4894
https://orcid.org/0000-0002-1260-777X
https://orcid.org/0000-0003-3681-0649
https://orcid.org/0000-0001-6332-5839
_version_ 1811083079353106432
author Apyan, Aram
Barbieri, Richard Alexander
Bauer, Gerry P
Busza, Wit
Cali, Ivan Amos
Di Matteo, Leonardo
Dutta, Valentina
Gomez-Ceballos, Guillelmo
Goncharov, Maxim
Gulhan, Doga Can
Klute, Markus
Lai, Yue Shi
Lee, Yen-Jie
Levin, Andrew Michael
Luckey Jr, P David
Ma, Teng
Paus, Christoph M. E.
Ralph, Duncan Kelley
Roland, Christof E
Roland, Gunther M
Stephans, George S. F.
Stoeckli, Fabian
Sumorok, Konstanty C
Velicanu, Dragos Alexandru
Veverka, Jan
Wyslouch, Boleslaw
Yang, Mingming
Zanetti, Marco
Wyslouch, Victoria
Chan, M.
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Apyan, Aram
Barbieri, Richard Alexander
Bauer, Gerry P
Busza, Wit
Cali, Ivan Amos
Di Matteo, Leonardo
Dutta, Valentina
Gomez-Ceballos, Guillelmo
Goncharov, Maxim
Gulhan, Doga Can
Klute, Markus
Lai, Yue Shi
Lee, Yen-Jie
Levin, Andrew Michael
Luckey Jr, P David
Ma, Teng
Paus, Christoph M. E.
Ralph, Duncan Kelley
Roland, Christof E
Roland, Gunther M
Stephans, George S. F.
Stoeckli, Fabian
Sumorok, Konstanty C
Velicanu, Dragos Alexandru
Veverka, Jan
Wyslouch, Boleslaw
Yang, Mingming
Zanetti, Marco
Wyslouch, Victoria
Chan, M.
author_sort Apyan, Aram
collection MIT
description The ratio of the top-quark branching fractions R=B(t→Wb)/B(t→Wq), where the denominator includes the sum over all down-type quarks (q=b,s,d), is measured in the t[¯ overt] dilepton final state with proton–proton collision data at √s=8 TeV from an integrated luminosity of 19.7 fb[superscript −1], collected with the CMS detector. In order to quantify the purity of the signal sample, the cross section is measured by fitting the observed jet multiplicity, thereby constraining the signal and background contributions. By counting the number of b jets per event, an unconstrained value of R=1.014±0.003(stat.)±0.032(syst.) is measured, in a good agreement with current precision measurements in electroweak and flavour sectors. A lower limit R > 0.955 at the 95% confidence level is obtained after requiring R≤1, and a lower limit on the Cabibbo–Kobayashi–Maskawa matrix element |V[subscript tb] | > 0.975 is set at 95% confidence level. The result is combined with a previous CMS measurement of the t-channel single-top-quark cross section to determine the top-quark total decay width, Γ[subscript t] =1.36±0.02(stat.) −0.11 +0.14 (syst.) GeV.
first_indexed 2024-09-23T12:20:33Z
format Article
id mit-1721.1/117038
institution Massachusetts Institute of Technology
last_indexed 2024-09-23T12:20:33Z
publishDate 2018
publisher Elsevier BV
record_format dspace
spelling mit-1721.1/1170382023-02-26T11:19:37Z Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV Apyan, Aram Barbieri, Richard Alexander Bauer, Gerry P Busza, Wit Cali, Ivan Amos Di Matteo, Leonardo Dutta, Valentina Gomez-Ceballos, Guillelmo Goncharov, Maxim Gulhan, Doga Can Klute, Markus Lai, Yue Shi Lee, Yen-Jie Levin, Andrew Michael Luckey Jr, P David Ma, Teng Paus, Christoph M. E. Ralph, Duncan Kelley Roland, Christof E Roland, Gunther M Stephans, George S. F. Stoeckli, Fabian Sumorok, Konstanty C Velicanu, Dragos Alexandru Veverka, Jan Wyslouch, Boleslaw Yang, Mingming Zanetti, Marco Wyslouch, Victoria Chan, M. Massachusetts Institute of Technology. Department of Physics Massachusetts Institute of Technology. Laboratory for Nuclear Science Apyan, Aram Barbieri, Richard Alexander Bauer, Gerry P Busza, Wit Cali, Ivan Amos Chan, Matthew Hans Di Matteo, Leonardo Dutta, Valentina Gomez-Ceballos, Guillelmo Goncharov, Maxim Gulhan, Doga Can Klute, Markus Lai, Yue Shi Lee, Yen-Jie Levin, Andrew Michael Luckey Jr, P David Ma, Teng Paus, Christoph M. E. Ralph, Duncan Kelley Roland, Christof E Roland, Gunther M Stephans, George S. F. Stoeckli, Fabian Sumorok, Konstanty C Velicanu, Dragos Alexandru Veverka, Jan Wyslouch, Boleslaw Yang, Mingming Zanetti, Marco Wyslouch, Victoria The ratio of the top-quark branching fractions R=B(t→Wb)/B(t→Wq), where the denominator includes the sum over all down-type quarks (q=b,s,d), is measured in the t[¯ overt] dilepton final state with proton–proton collision data at √s=8 TeV from an integrated luminosity of 19.7 fb[superscript −1], collected with the CMS detector. In order to quantify the purity of the signal sample, the cross section is measured by fitting the observed jet multiplicity, thereby constraining the signal and background contributions. By counting the number of b jets per event, an unconstrained value of R=1.014±0.003(stat.)±0.032(syst.) is measured, in a good agreement with current precision measurements in electroweak and flavour sectors. A lower limit R > 0.955 at the 95% confidence level is obtained after requiring R≤1, and a lower limit on the Cabibbo–Kobayashi–Maskawa matrix element |V[subscript tb] | > 0.975 is set at 95% confidence level. The result is combined with a previous CMS measurement of the t-channel single-top-quark cross section to determine the top-quark total decay width, Γ[subscript t] =1.36±0.02(stat.) −0.11 +0.14 (syst.) GeV. National Science Foundation (U.S.) United States. Department of Energy 2018-07-20T19:35:44Z 2018-07-20T19:35:44Z 2014-07 2014-06 2018-05-11T15:28:15Z Article http://purl.org/eprint/type/JournalArticle 0370-2693 http://hdl.handle.net/1721.1/117038 Khachatryan, V., et al. “Measurement of the Ratio B (t → Wb/B (t → Wq) in Pp Collisions at √s = 8 TeV.” Physics Letters B, vol. 736, Sept. 2014, pp. 33–57. © 2014 The Authors https://orcid.org/0000-0002-9418-6656 https://orcid.org/0000-0002-7945-005X https://orcid.org/0000-0002-3831-9071 https://orcid.org/0000-0002-2822-3375 https://orcid.org/0000-0001-9236-6621 https://orcid.org/0000-0002-0869-5631 https://orcid.org/0000-0003-1486-606X https://orcid.org/0000-0003-2593-7767 https://orcid.org/0000-0002-1136-6900 https://orcid.org/0000-0002-6047-4211 https://orcid.org/0000-0001-8983-2169 https://orcid.org/0000-0003-3106-4894 https://orcid.org/0000-0002-1260-777X https://orcid.org/0000-0003-3681-0649 https://orcid.org/0000-0001-6332-5839 http://dx.doi.org/10.1016/J.PHYSLETB.2014.06.076 Physics Letters B Attribution 4.0 International (CC BY 4.0) https://creativecommons.org/licenses/by/4.0/ application/pdf Elsevier BV Physics Letters B
spellingShingle Apyan, Aram
Barbieri, Richard Alexander
Bauer, Gerry P
Busza, Wit
Cali, Ivan Amos
Di Matteo, Leonardo
Dutta, Valentina
Gomez-Ceballos, Guillelmo
Goncharov, Maxim
Gulhan, Doga Can
Klute, Markus
Lai, Yue Shi
Lee, Yen-Jie
Levin, Andrew Michael
Luckey Jr, P David
Ma, Teng
Paus, Christoph M. E.
Ralph, Duncan Kelley
Roland, Christof E
Roland, Gunther M
Stephans, George S. F.
Stoeckli, Fabian
Sumorok, Konstanty C
Velicanu, Dragos Alexandru
Veverka, Jan
Wyslouch, Boleslaw
Yang, Mingming
Zanetti, Marco
Wyslouch, Victoria
Chan, M.
Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV
title Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV
title_full Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV
title_fullStr Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV
title_full_unstemmed Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV
title_short Measurement of the ratio B(t → Wb)/B(t → Wq) in pp collisions at √s = 8 TeV
title_sort measurement of the ratio b t wb b t wq in pp collisions at √s 8 tev
url http://hdl.handle.net/1721.1/117038
https://orcid.org/0000-0002-9418-6656
https://orcid.org/0000-0002-7945-005X
https://orcid.org/0000-0002-3831-9071
https://orcid.org/0000-0002-2822-3375
https://orcid.org/0000-0001-9236-6621
https://orcid.org/0000-0002-0869-5631
https://orcid.org/0000-0003-1486-606X
https://orcid.org/0000-0003-2593-7767
https://orcid.org/0000-0002-1136-6900
https://orcid.org/0000-0002-6047-4211
https://orcid.org/0000-0001-8983-2169
https://orcid.org/0000-0003-3106-4894
https://orcid.org/0000-0002-1260-777X
https://orcid.org/0000-0003-3681-0649
https://orcid.org/0000-0001-6332-5839
work_keys_str_mv AT apyanaram measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT barbieririchardalexander measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT bauergerryp measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT buszawit measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT caliivanamos measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT dimatteoleonardo measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT duttavalentina measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT gomezceballosguillelmo measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT goncharovmaxim measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT gulhandogacan measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT klutemarkus measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT laiyueshi measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT leeyenjie measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT levinandrewmichael measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT luckeyjrpdavid measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT mateng measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT pauschristophme measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT ralphduncankelley measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT rolandchristofe measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT rolandguntherm measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT stephansgeorgesf measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT stoecklifabian measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT sumorokkonstantyc measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT velicanudragosalexandru measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT veverkajan measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT wyslouchboleslaw measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT yangmingming measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT zanettimarco measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT wyslouchvictoria measurementoftheratiobtwbbtwqinppcollisionsats8tev
AT chanm measurementoftheratiobtwbbtwqinppcollisionsats8tev