Measurement of the top quark mass using proton-proton data at √s=7 and 8 TeV

@article{Khachatryan2016MeasurementOT,
  title={Measurement of the top quark mass using proton-proton data at √s=7 and 8 TeV},
  author={Vardan Khachatryan and Marc Besançon and Fabrice Couderc and Marc D{\'e}jardin and Daniel Denegri and Bernard Fabbro and J{\'e}r{\^o}me Faure and Carlotta Favaro and F. Ferri and Serguei Ganjour and Alain Givernaud and Philippe Gras and Gautier Hamel de Monchenault and Patrick Jarry and E. Locci and Martina Machet and Julie Malcl{\`e}s and John Rander and Andr{\'e} Rosowsky and Maksym Titov and Amina Zghiche and Iurii Antropov and Stephanie Baffioni and Florian Beaudette and Philippe Busson and Luca Cadamuro and Emilien Chapon and Claude Charlot and Torsten Dahms and Olivier Davignon and Nicolas Filipovic and Alice Florent and R. Granier de Cassagnac and Stanislav Lisniak and Luca Mastrolorenzo and Ivo Nicolas Naranjo and Matthew Nguyen and Christophe Ochando and Giacomo Ortona and Pascal Paganini and Philipp Pigard and Simon Regnard and Roberto Salerno and J. B. Sauvan and Yves Sirois and Thomas Strebler and Yetkin Yilmaz and Alexandre Zabi and J.-L. Agram and J{\'e}r{\'e}my Andrea and Alexandre Aubin and Daniel Bloch and J. M. Brom and Michael Buttignol and Eric Christian Chabert and Nicolas Chanon and Caroline Collard and Eric Conte and Xavier Coubez and J. Ch. Fontaine and Denis Gel{\'e} and Ulrich Goerlach and Christophe Goetzmann and A. C. Le Bihan and Jeremie A. Merlin and Kirill Skovpen and P. Van Hove and S{\'e}bastien Gadrat and Stephanie Beauceron and Colin Bernet and Gaelle Boudoul and E. Bouvier and C. A. Carrillo Montoya and Roberto Chierici and Didier Contardo and Benoit Courbon and Pierre Depasse and Houmani El Mamouni and Jiawei Fan and Jean Fay and Susan Gascon and Maxime Gouzevitch and Bernard Ille and François Lagarde and I. B. Laktineh and Morgan Lethuillier and Laurent Mirabito and A. L. Pequegnot and St{\'e}phane Perri{\`e}s and J. D. Ruiz Alvarez and David Sabes and Louis Sgandurra and Viola Sordini and Muriel Vander Donckt and Patrice Verdier and Sebastien Viret},
  journal={Physical Review D},
  year={2016},
  volume={93},
  pages={072004}
}
A new set of measurements of the top quark mass are presented, based on the proton-proton data recorded by the CMS experiment at the LHC at sqrt(s) = 8 TeV corresponding to a luminosity of 19.7 inverse femtobarns. The top quark mass is measured using the lepton+jets, all-jets and dilepton decay channels, giving values of 172.35 +/- 0.16 (stat) +/- 0.48 (syst) GeV, 172.32 +/- 0.25 (stat) +/- 0.59 (syst) GeV, and 172.82 +/- 0.19 (stat) +/- 1.22 (syst) GeV, respectively. When combined with the… 

Measurement of the top quark mass in the tt → lepton+jets channel from √s=8 TeV ATLAS data and combination with previous results

The top quark mass is measured using a template method in the t t̄ → lepton + jets channel (lepton is e or μ) using ATLAS data recorded in 2012 at the LHC. The data were taken at a proton–proton

Measurement of the top quark mass using single top quark events in proton-proton collisions at sqrt(s) = 8 TeV

A measurement of the top quark mass is reported in events containing a single top quark produced via the electroweak t channel. The analysis is performed using data from proton-proton collisions

University of Birmingham Measurement of the top quark mass in the tt ̄ lepton+jets channel from s=8 TeV ATLAS data and combination with previous results

The top quark mass is measured using a template method in the t t̄ → lepton + jets channel (lepton is e or μ) using ATLAS data recorded in 2012 at the LHC. The data were taken at a proton–proton

Measurement of the top quark mass using lepton transverse momenta with the ATLAS detector at √s = 8 TeV

The mass of the top quark is determined in proton-proton collisions at a centreof-mass energy of 8 TeV, recorded by the ATLAS experiment at the LHC. For the measurement, tt̄ events with lepton+jets

Direct Top Quark Decay Width Measurement in the tt Lepton+Jets Channel at 8 TeV with the ATLAS Experiment

This paper presents a direct measurement of the decay width of the top quark using t ¯ t events in the lep-ton+jets final state. The data sample was collected by the ATLAS detector at the LHC in

Measurement of the top quark mass using charged particles in pp collisions at s√=8 TeV

A novel technique for measuring the mass of the top quark that uses only the kinematic properties of its charged decay products is presented. Top quark pair events with final states with one or two

Measurement of the top quark mass with lepton+jets final states using pp collisions at $\sqrt{s} =$ 13 TeV

The mass of the top quark is measured using a sample of t t events collected by the CMS detector using proton-proton collisions at √ s = 13 TeV at the CERN LHC. Events are selected with one isolated

Measurement of the top quark mass in the t t̄ → lepton + jets channel from √ s = 8 TeV ATLAS data and combination with previous results

The top quark mass is measured using a template method in the t t̄ → lepton + jets channel (lepton is e or μ) using ATLAS data recorded in 2012 at the LHC. The data were taken at a proton–proton

Measurement of the top quark mass in the t t̄ → lepton + jets channel from √ s = 8 TeV ATLAS data and combination with previous results

The top quark mass is measured using a template method in the t t̄ → lepton + jets channel (lepton is e or μ) using ATLAS data recorded in 2012 at the LHC. The data were taken at a proton–proton

Measurement of the top quark mass in the t(t)over-bar -> lepton plus jets channel from root s=8 TeV ATLAS data and combination with previous results ATLAS

The top quark mass is measured using a template method in the t t̄ → lepton + jets channel (lepton is e or μ) using ATLAS data recorded in 2012 at the LHC. The data were taken at a proton–proton
...

References

SHOWING 1-10 OF 114 REFERENCES

Measurement of the top-quark mass in ttˉ events with dilepton final states in pp collisions at s√=7 TeV

The top-quark mass is measured in proton-proton collisions at s√=7 TeV using a data sample corresponding to an integrated luminosity of 5.0 fb−1 collected by the CMS experiment at the LHC. The

Direct Measurement of the Top Quark Mass at D0

We determine the top quark mass m t using tt pairs produced in the DØ detector by √ s = 1 . 8 TeV pp collisions in a 125 pb − 1 exposure at the Fermilab Tevatron. We make a two constraint fit to m t

Measurement of the differential cross section for top quark pair production in pp collisions at √s = 8 TeV

: The normalized differential cross section for top quark pair ( t ¯ t ) production is measured in pp collisions at a centre-of-mass energy of 8 TeV at the CERN LHC using the CMS detector in data

Measurement of the top quark mass in the tt¯→lepton+jets and tt¯→dilepton channels using s=7 TeV ATLAS data

The top quark mass was measured in the channels t ¯ t → lepton+jets and t ¯ t → dilepton (lepton = e , μ ) based on ATLAS data recorded in 2011. The data were taken at the LHC with a proton–proton

First combination of Tevatron and LHC measurements of the top-quark mass

We present a combination of measurements of the mass of the top quark, $m_{\rm top}$, performed by the CDF and D0 experiments at the Tevatron collider and the ATLAS and CMS experiments at the Large

Study of the fragmentation of b quarks into B mesons at the Z peak

The electroweak fit of the standard model after the discovery of a new boson at the LHC

In view of the discovery of a new boson by the ATLAS and CMS Collaborations at the LHC, we present an update of the global Standard Model (SM) fit to electroweak precision data. Assuming the new

Performance of electron reconstruction and selection with the CMS detector in proton-proton collisions at √s=8 TeV

The performance and strategies used in electron reconstruction and selection at CMS are presented based on data corresponding to an integrated luminosity of 19.7 inverse femtobarns, collected in

Total top-quark pair-production cross section at hadron colliders through O(αS(4)).

The result derived in this Letter completes the set of NNLO QCD corrections to the total top pair-production cross section at hadron colliders and allows a new level of scrutiny in parton distribution functions and new physics searches.

Measurement of the underlying event activity at the LHC with $ \sqrt {s} = 7 $ TeV and comparison with $ \sqrt {s} = 0.9 $ TeV

A measurement of the underlying activity in events with a jet of transverse momentum in the several GeV region is performed in proton-proton collisions at $ \sqrt {s} = 0.9 $ and 7 TeV, using data
...