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The Higgs transverse momentum spectrum with finite quark masses beyond leading order

We apply the leading-log high-energy resummation technique recently derived by some of us to the transverse momentum (pt) distribution for production of a Higgs boson in gluon fusion. We use our results to obtain information on mass-dependent corrections to this observable, which is only known at le...

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Detalles Bibliográficos
Autores principales: Caola, Fabrizio, Forte, Stefano, Marzani, Simone, Muselli, Claudio, Vita, Gherardo
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP08(2016)150
http://cds.cern.ch/record/2161327
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author Caola, Fabrizio
Forte, Stefano
Marzani, Simone
Muselli, Claudio
Vita, Gherardo
author_facet Caola, Fabrizio
Forte, Stefano
Marzani, Simone
Muselli, Claudio
Vita, Gherardo
author_sort Caola, Fabrizio
collection CERN
description We apply the leading-log high-energy resummation technique recently derived by some of us to the transverse momentum (pt) distribution for production of a Higgs boson in gluon fusion. We use our results to obtain information on mass-dependent corrections to this observable, which is only known at leading order when exact mass dependence is included. In the low pt region we discuss the all-order exponentiation of collinear bottom mass logarithms. In the high pt region we show that the infinite top mass approximation loses accuracy as a power of pt, while the accuracy of the high-energy approximation is approximately constant as pt grows. We argue that a good approximation to the NLO result for pt >~200 GeV can be obtained by combining the full LO result with a K-factor computed using the high-energy approximation.
id cern-2161327
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2016
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spelling cern-21613272022-08-10T12:40:49Zdoi:10.1007/JHEP08(2016)150http://cds.cern.ch/record/2161327engCaola, FabrizioForte, StefanoMarzani, SimoneMuselli, ClaudioVita, GherardoThe Higgs transverse momentum spectrum with finite quark masses beyond leading orderParticle Physics - PhenomenologyWe apply the leading-log high-energy resummation technique recently derived by some of us to the transverse momentum (pt) distribution for production of a Higgs boson in gluon fusion. We use our results to obtain information on mass-dependent corrections to this observable, which is only known at leading order when exact mass dependence is included. In the low pt region we discuss the all-order exponentiation of collinear bottom mass logarithms. In the high pt region we show that the infinite top mass approximation loses accuracy as a power of pt, while the accuracy of the high-energy approximation is approximately constant as pt grows. We argue that a good approximation to the NLO result for pt >~200 GeV can be obtained by combining the full LO result with a K-factor computed using the high-energy approximation.We apply the leading-log high-energy resummation technique recently derived by some of us to the transverse momentum distribution for production of a Higgs boson in gluon fusion. We use our results to obtain information on mass-dependent corrections to this observable, which is only known at leading order when exact mass dependence is included. In the low p$_{T}$ region we discuss the all-order exponentiation of collinear bottom mass logarithms. In the high p$_{T}$ region we show that the infinite top mass approximation loses accuracy as a power of p$_{T}$, while the accuracy of the high-energy approximation is approximately constant as p$_{T}$ grows. We argue that a good approximation to the NLO result for p$_{T}$ ≳ 200 GeV can be obtained by combining the full LO result with a K-factor computed using the high-energy approximation.We apply the leading-log high-energy resummation technique recently derived by some of us to the transverse momentum (pt) distribution for production of a Higgs boson in gluon fusion. We use our results to obtain information on mass-dependent corrections to this observable, which is only known at leading order when exact mass dependence is included. In the low pt region we discuss the all-order exponentiation of collinear bottom mass logarithms. In the high pt region we show that the infinite top mass approximation loses accuracy as a power of pt, while the accuracy of the high-energy approximation is approximately constant as pt grows. We argue that a good approximation to the NLO result for pt >~200 GeV can be obtained by combining the full LO result with a K-factor computed using the high-energy approximation.arXiv:1606.04100CERN-TH-2016-139TIF-UNIMI-2016-4MIT-CTP-4799CERN-TH-2016-139TIF-UNIMI-2016-4MIT-CTP-4799oai:cds.cern.ch:21613272016-06-13
spellingShingle Particle Physics - Phenomenology
Caola, Fabrizio
Forte, Stefano
Marzani, Simone
Muselli, Claudio
Vita, Gherardo
The Higgs transverse momentum spectrum with finite quark masses beyond leading order
title The Higgs transverse momentum spectrum with finite quark masses beyond leading order
title_full The Higgs transverse momentum spectrum with finite quark masses beyond leading order
title_fullStr The Higgs transverse momentum spectrum with finite quark masses beyond leading order
title_full_unstemmed The Higgs transverse momentum spectrum with finite quark masses beyond leading order
title_short The Higgs transverse momentum spectrum with finite quark masses beyond leading order
title_sort higgs transverse momentum spectrum with finite quark masses beyond leading order
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP08(2016)150
http://cds.cern.ch/record/2161327
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