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

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Precision measurement of the top quark mass in $lepton+jets$ final states. / D0 Collaboration.
In: Physical review letters, Vol. 113, No. 3, 032002, 17.07.2014.

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

Harvard

D0 Collaboration 2014, 'Precision measurement of the top quark mass in $lepton+jets$ final states', Physical review letters, vol. 113, no. 3, 032002. https://doi.org/10.1103/PhysRevLett.113.032002

APA

D0 Collaboration (2014). Precision measurement of the top quark mass in $lepton+jets$ final states. Physical review letters, 113(3), Article 032002. https://doi.org/10.1103/PhysRevLett.113.032002

Vancouver

D0 Collaboration. Precision measurement of the top quark mass in $lepton+jets$ final states. Physical review letters. 2014 Jul 17;113(3):032002. doi: 10.1103/PhysRevLett.113.032002

Author

D0 Collaboration. / Precision measurement of the top quark mass in $lepton+jets$ final states. In: Physical review letters. 2014 ; Vol. 113, No. 3.

Bibtex

@article{5a926f045c7d4307b201ee2ecb0c31ad,
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 = "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 {Besanifmmode {\c c}else {\c c}on}, M. 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} 2014 American Physical Society",
year = "2014",
month = jul,
day = "17",
doi = "10.1103/PhysRevLett.113.032002",
language = "English",
volume = "113",
journal = "Physical review letters",
issn = "1079-7114",
publisher = "American Physical Society",
number = "3",

}

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 - © 2014 American Physical Society

PY - 2014/7/17

Y1 - 2014/7/17

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/PhysRevLett.113.032002

DO - 10.1103/PhysRevLett.113.032002

M3 - Journal article

VL - 113

JO - Physical review letters

JF - Physical review letters

SN - 1079-7114

IS - 3

M1 - 032002

ER -