Home > Research > Publications & Outputs > Precision measurement of the top-quark mass in ...

Research

Associated organisational units

Electronic data

  • PhysRevD.91.112003

    Rights statement: © 2015 American Physical Society

    Final published version, 2.95 MB, PDF document

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

Links

Text available via DOI:

View graph of relations

Precision measurement of the top-quark mass in lepton+jets final states

Research output: Contribution to Journal/Magazine › Journal article › peer-review

Published

Standard

Precision measurement of the top-quark mass in lepton+jets final states. / D0 Collaboration.
In: Physical Review D, Vol. 91, No. 11, 112003, 04.06.2015.

Research output: Contribution to Journal/Magazine › Journal article › peer-review

Harvard

D0 Collaboration 2015, 'Precision measurement of the top-quark mass in lepton+jets final states', Physical Review D, vol. 91, no. 11, 112003. https://doi.org/10.1103/PhysRevD.91.112003

APA

D0 Collaboration (2015). Precision measurement of the top-quark mass in lepton+jets final states. Physical Review D, 91(11), Article 112003. https://doi.org/10.1103/PhysRevD.91.112003

Vancouver

D0 Collaboration. Precision measurement of the top-quark mass in lepton+jets final states. Physical Review D. 2015 Jun 4;91(11):112003. Epub 2015 Jun 1. doi: 10.1103/PhysRevD.91.112003

Author

D0 Collaboration. / Precision measurement of the top-quark mass in lepton+jets final states. In: Physical Review D. 2015 ; Vol. 91, No. 11.

Bibtex

@article{2609a8df73224b16b9dac53742f78dd5,
title = "Precision measurement of the top-quark mass in lepton+jets final states",
abstract = "We measure the mass of the top quark in lepton+jets final states using the full sample of pp¯ collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at s√=1.96  TeV, corresponding to 9.7  fb−1 of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from tt¯ production or background. The overall jet energy scale is constrained in situ by the mass of the W boson. We measure mt=174.98±0.76  GeV. This constitutes the most precise single measurement of the top-quark mass.",
author = "Abazov, {V. M.} and B. Abbott and Acharya, {B. S.} and M. Adams and T. Adams and Agnew, {J. P.} and Alexeev, {G. D.} 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 Bandurin, {D. V.} and S. Banerjee and E. Barberis and P. Baringer and Bartlett, {J. F.} and U. Bassler and V. Bazterra and A. Bean and M. Begalli and L. Bellantoni and Beri, {S. B.} and G. Bernardi and R. Bernhard and I. Bertram and {Besanifmmode {\c c}else {\c c}on}, M. and R. Beuselinck and Bhat, {P. C.} and S. Bhatia and V. Bhatnagar and G. Blazey and S. Blessing and K. Bloom and A. Boehnlein and D. Boline and Boos, {E. E.} and G. Borissov and M. Borysova and A. Brandt and O. Brandt and H. Fox and D. Price and Ratoff, {P. N.} and A. Ross and Williams, {M. R. J.} and {D0 Collaboration}",
note = "{\textcopyright} 2015 American Physical Society ",
year = "2015",
month = jun,
day = "4",
doi = "10.1103/PhysRevD.91.112003",
language = "English",
volume = "91",
journal = "Physical Review D",
issn = "1550-7998",
publisher = "American Physical Society",
number = "11",

}

RIS

TY - JOUR

T1 - Precision measurement of the top-quark mass in lepton+jets final states

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 - Besanifmmode çelse çon, 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 American Physical Society

PY - 2015/6/4

Y1 - 2015/6/4

N2 - We measure the mass of the top quark in lepton+jets final states using the full sample of pp¯ collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at s√=1.96  TeV, corresponding to 9.7  fb−1 of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from tt¯ production or background. The overall jet energy scale is constrained in situ by the mass of the W boson. We measure mt=174.98±0.76  GeV. This constitutes the most precise single measurement of the top-quark mass.

AB - We measure the mass of the top quark in lepton+jets final states using the full sample of pp¯ collision data collected by the D0 experiment in Run II of the Fermilab Tevatron Collider at s√=1.96  TeV, corresponding to 9.7  fb−1 of integrated luminosity. We use a matrix element technique that calculates the probabilities for each event to result from tt¯ production or background. The overall jet energy scale is constrained in situ by the mass of the W boson. We measure mt=174.98±0.76  GeV. This constitutes the most precise single measurement of the top-quark mass.

U2 - 10.1103/PhysRevD.91.112003

DO - 10.1103/PhysRevD.91.112003

M3 - Journal article

VL - 91

JO - Physical Review D

JF - Physical Review D

SN - 1550-7998

IS - 11

M1 - 112003

ER -