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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...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2016
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP08(2016)150 http://cds.cern.ch/record/2161327 |
_version_ | 1780950951117455360 |
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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 |
record_format | invenio |
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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