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The Top Quark Mass at the LHC

I briefly discuss some theoretical aspects of top mass measurements at the LHC. In particular, I illustrate a recent theoretical study performed using next-to-leading order (NLO) calculations interfaced to shower generators (NLO+PS) of increasing accuracy, interfaced to both Pythia8 and Herwig7 Mont...

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Autor principal: Nason, Paolo
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:http://cds.cern.ch/record/2300287
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author Nason, Paolo
author_facet Nason, Paolo
author_sort Nason, Paolo
collection CERN
description I briefly discuss some theoretical aspects of top mass measurements at the LHC. In particular, I illustrate a recent theoretical study performed using next-to-leading order (NLO) calculations interfaced to shower generators (NLO+PS) of increasing accuracy, interfaced to both Pythia8 and Herwig7 Monte Carlo generators.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-23002872020-12-14T13:46:17Zhttp://cds.cern.ch/record/2300287engNason, PaoloThe Top Quark Mass at the LHChep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyI briefly discuss some theoretical aspects of top mass measurements at the LHC. In particular, I illustrate a recent theoretical study performed using next-to-leading order (NLO) calculations interfaced to shower generators (NLO+PS) of increasing accuracy, interfaced to both Pythia8 and Herwig7 Monte Carlo generators.I briefly discuss some theoretical aspects of top mass measurements at the LHC.In particular, I illustrate recent theoretical studies performed using next-to-leading order (NLO) calculations interfaced to shower generators (NLO+PS) ofincreasing accuracy. I consider three generators: one that has NLO accuracy onlyat the production stage, and implements spin correlations in an approximate way;one that implements NLO corrections also in decay, and includes exact spincorrelations in the narrow-width limit; and one that includes NLO corrections inproduction and decays, also taking care of finite width, non-resonantcontributions and interference of radiation in production and decay. Animportant goal of the LHC top-physics program is the measurement of its mass.Since the Higgs mass is known with high precision, improvements of both the Wand top mass measurements may lead to a refinement of the Electro-Weak precisiontests 1, 2). The current precision of the W mass measurement, of about 15 MeV,would match a precision on the top mass of about 2.4 GeV. There is some tensionat present between the value of the top mass obtained indirectly throughelectro-weak fits 1) , 176.7 ± 2.1 GeV, and the direct determinations, with thevalue of 173.34 ± 0.76 GeV from the latest combination 3) , and with latermeasurements yielding values smaller by about 1 GeV 4, 5, 6, 7). 1 The value ofthe top mass is also relevant for the issue of vacuum stability in the StandardModel 10, 11, 12). Direct measurements are now well below the instabilityregion, while the central value extracted from electro-weak fits is near itsedge. The only conclusion that one can draw from these results is that noindication of new physics scales below the Plank scale arises from the vacuum 1For recent reviews of top-mass measurements by the ATLAS and CMS collaborationssee Refs. 8) and 9) from these proceedings.CERN-TH-2018-008arXiv:1801.04826oai:cds.cern.ch:23002872017
spellingShingle hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
Nason, Paolo
The Top Quark Mass at the LHC
title The Top Quark Mass at the LHC
title_full The Top Quark Mass at the LHC
title_fullStr The Top Quark Mass at the LHC
title_full_unstemmed The Top Quark Mass at the LHC
title_short The Top Quark Mass at the LHC
title_sort top quark mass at the lhc
topic hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
url http://cds.cern.ch/record/2300287
work_keys_str_mv AT nasonpaolo thetopquarkmassatthelhc
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