Home > Research > Publications & Outputs > Precise measurement of the top quark mass in di...

Electronic data

  • 1_s2.0_S037026931500845X_main

    Rights statement: © 2015 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3

    Final published version, 502 KB, PDF document

    Available under license: CC BY: Creative Commons Attribution 4.0 International License

Links

Text available via DOI:

View graph of relations

Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Published

Standard

Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting. / D0 Collaboration.
In: Physics Letters B, Vol. 752, 10.01.2016, p. 18-26.

Research output: Contribution to Journal/MagazineJournal articlepeer-review

Harvard

APA

Vancouver

D0 Collaboration. Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting. Physics Letters B. 2016 Jan 10;752:18-26. doi: 10.1016/j.physletb.2015.10.086

Author

D0 Collaboration. / Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting. In: Physics Letters B. 2016 ; Vol. 752. pp. 18-26.

Bibtex

@article{088adb6881bd4a5f8c6867d99925e0e1,
title = "Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting",
abstract = "We measure the top quark mass in dilepton final states of top-antitop events in proton-antiproton collisions at sqrt(s) = 1.96 TeV, using data corresponding to an integrated luminosity of 9.7 fb^-1 at the Fermilab Tevatron Collider. The analysis features a comprehensive optimization of the neutrino weighting method to minimize the statistical uncertainties. We also improve the calibration of jet energies using the calibration determined in top-antitop to lepton+jets events, which reduces the otherwise limiting systematic uncertainty from the jet energy scale. The measured top quark mass is mt = 173.32 +/- 1.36(stat) +/- 0.85(syst) GeV.",
author = "V.M. Abazov and B. Abbott and B.S. Acharya and M. Adams and T. Adams and J.P. Agnew and G.D. Alexeev and G. Alkhazov and A. Alton and A. Askew and S. Atkins and K. Augsten and C. Avila and F. Badaud and L. Bagby and B. Baldin and D.V. Bandurin and S. Banerjee and E. Barberis and P. Baringer and J.F. Bartlett and U. Bassler and V. Bazterra and A. Bean and M. Begalli and L. Bellantoni and S.B. Beri and G. Bernardi and R. Bernhard and I. Bertram and M. Besan√{\ss}on and R. Beuselinck and P.C. Bhat and S. Bhatia and V. Bhatnagar and G. Blazey and S. Blessing and K. Bloom and A. Boehnlein and D. Boline and E.E. Boos and G. Borissov and M. Borysova and A. Brandt and O. Brandt and H. Fox and D. Price and P.N. Ratoff and A. Ross and M.R.J. Williams and {D0 Collaboration}",
note = "{\textcopyright} 2015 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3",
year = "2016",
month = jan,
day = "10",
doi = "10.1016/j.physletb.2015.10.086",
language = "English",
volume = "752",
pages = "18--26",
journal = "Physics Letters B",
issn = "0370-2693",
publisher = "ELSEVIER SCIENCE BV",

}

RIS

TY - JOUR

T1 - Precise measurement of the top quark mass in dilepton decays using optimized neutrino weighting

AU - Abazov, V.M.

AU - Abbott, B.

AU - Acharya, B.S.

AU - Adams, M.

AU - Adams, T.

AU - Agnew, J.P.

AU - Alexeev, G.D.

AU - Alkhazov, G.

AU - Alton, A.

AU - Askew, A.

AU - Atkins, S.

AU - Augsten, K.

AU - Avila, C.

AU - Badaud, F.

AU - Bagby, L.

AU - Baldin, B.

AU - Bandurin, D.V.

AU - Banerjee, S.

AU - Barberis, E.

AU - Baringer, P.

AU - Bartlett, J.F.

AU - Bassler, U.

AU - Bazterra, V.

AU - Bean, A.

AU - Begalli, M.

AU - Bellantoni, L.

AU - Beri, S.B.

AU - Bernardi, G.

AU - Bernhard, R.

AU - Bertram, I.

AU - Besançon, M.

AU - Beuselinck, R.

AU - Bhat, P.C.

AU - Bhatia, S.

AU - Bhatnagar, V.

AU - Blazey, G.

AU - Blessing, S.

AU - Bloom, K.

AU - Boehnlein, A.

AU - Boline, D.

AU - Boos, E.E.

AU - Borissov, G.

AU - Borysova, M.

AU - Brandt, A.

AU - Brandt, O.

AU - Fox, H.

AU - Price, D.

AU - Ratoff, P.N.

AU - Ross, A.

AU - Williams, M.R.J.

AU - D0 Collaboration

N1 - © 2015 The Authors. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3

PY - 2016/1/10

Y1 - 2016/1/10

N2 - We measure the top quark mass in dilepton final states of top-antitop events in proton-antiproton collisions at sqrt(s) = 1.96 TeV, using data corresponding to an integrated luminosity of 9.7 fb^-1 at the Fermilab Tevatron Collider. The analysis features a comprehensive optimization of the neutrino weighting method to minimize the statistical uncertainties. We also improve the calibration of jet energies using the calibration determined in top-antitop to lepton+jets events, which reduces the otherwise limiting systematic uncertainty from the jet energy scale. The measured top quark mass is mt = 173.32 +/- 1.36(stat) +/- 0.85(syst) GeV.

AB - We measure the top quark mass in dilepton final states of top-antitop events in proton-antiproton collisions at sqrt(s) = 1.96 TeV, using data corresponding to an integrated luminosity of 9.7 fb^-1 at the Fermilab Tevatron Collider. The analysis features a comprehensive optimization of the neutrino weighting method to minimize the statistical uncertainties. We also improve the calibration of jet energies using the calibration determined in top-antitop to lepton+jets events, which reduces the otherwise limiting systematic uncertainty from the jet energy scale. The measured top quark mass is mt = 173.32 +/- 1.36(stat) +/- 0.85(syst) GeV.

U2 - 10.1016/j.physletb.2015.10.086

DO - 10.1016/j.physletb.2015.10.086

M3 - Journal article

VL - 752

SP - 18

EP - 26

JO - Physics Letters B

JF - Physics Letters B

SN - 0370-2693

ER -