Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO

Abstract Measurements of Higgs boson processes by the ATLAS and CMS experiments at the LHC use Simplified Template Cross Sections (STXS) as a common framework for the combination of measurements in different decay channels and their further interpretation, e.g. to measure Higgs couplings. The differ...

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Main Authors: Pedro Cal, Matthew A. Lim, Darren J. Scott, Frank J. Tackmann, Wouter J. Waalewijn
Format: Article
Language:English
Published: SpringerOpen 2025-03-01
Series:Journal of High Energy Physics
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Online Access:https://doi.org/10.1007/JHEP03(2025)155
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author Pedro Cal
Matthew A. Lim
Darren J. Scott
Frank J. Tackmann
Wouter J. Waalewijn
author_facet Pedro Cal
Matthew A. Lim
Darren J. Scott
Frank J. Tackmann
Wouter J. Waalewijn
author_sort Pedro Cal
collection DOAJ
description Abstract Measurements of Higgs boson processes by the ATLAS and CMS experiments at the LHC use Simplified Template Cross Sections (STXS) as a common framework for the combination of measurements in different decay channels and their further interpretation, e.g. to measure Higgs couplings. The different Higgs production processes are measured in predefined kinematic regions — the STXS bins — requiring precise theory predictions for each individual bin. In gluon-fusion Higgs production a main division is into 0-jet, 1-jet, and ≥ 2-jet bins, which are further subdivided in bins of the Higgs transverse momentum p T H $$ {p}_T^H $$ . Requiring a fixed number of jets induces logarithms ln p T cut / Q $$ {p}_T^{\textrm{cut}}/Q $$ in the cross section where p T cut $$ {p}_T^{\textrm{cut}} $$ is the jet-p T threshold and Q ∼ p T H $$ {p}_T^H $$ ∼ m H the hard-interaction scale. These jet-veto logarithms can be resummed to all orders in perturbation theory to achieve the highest possible perturbative precision. We provide state-of-the art predictions for the p T H $$ {p}_T^H $$ spectrum in exclusive H+1-jet production and the corresponding H+1-jet STXS bins in the kinematic regime p T cut $$ {p}_T^{\textrm{cut}} $$ ≪ p T H $$ {p}_T^H $$ ∼ m H . We carry out the resummation at NNLL ′ accuracy, using theory nuisance parameters to account for the few unknown ingredients at this order, and match to full NNLO. We revisit the jet-veto factorization for this process and find that it requires refactorizing the total soft function into a global and soft-collinear contribution in order to fully account for logarithms of the signal jet radius. The leading nonglobal logarithms are also included, though they are numerically small for the region of phenomenological interest.
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spelling doaj-art-400a998c21434016917b8215e6b7298b2025-08-20T02:17:01ZengSpringerOpenJournal of High Energy Physics1029-84792025-03-012025315010.1007/JHEP03(2025)155Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLOPedro Cal0Matthew A. Lim1Darren J. Scott2Frank J. Tackmann3Wouter J. Waalewijn4Deutsches Elektronen-Synchrotron DESYDepartment of Physics and Astronomy, University of SussexMax Planck Institute for PhysicsDeutsches Elektronen-Synchrotron DESYInstitute for Theoretical Physics Amsterdam and Delta Institute for Theoretical Physics, University of AmsterdamAbstract Measurements of Higgs boson processes by the ATLAS and CMS experiments at the LHC use Simplified Template Cross Sections (STXS) as a common framework for the combination of measurements in different decay channels and their further interpretation, e.g. to measure Higgs couplings. The different Higgs production processes are measured in predefined kinematic regions — the STXS bins — requiring precise theory predictions for each individual bin. In gluon-fusion Higgs production a main division is into 0-jet, 1-jet, and ≥ 2-jet bins, which are further subdivided in bins of the Higgs transverse momentum p T H $$ {p}_T^H $$ . Requiring a fixed number of jets induces logarithms ln p T cut / Q $$ {p}_T^{\textrm{cut}}/Q $$ in the cross section where p T cut $$ {p}_T^{\textrm{cut}} $$ is the jet-p T threshold and Q ∼ p T H $$ {p}_T^H $$ ∼ m H the hard-interaction scale. These jet-veto logarithms can be resummed to all orders in perturbation theory to achieve the highest possible perturbative precision. We provide state-of-the art predictions for the p T H $$ {p}_T^H $$ spectrum in exclusive H+1-jet production and the corresponding H+1-jet STXS bins in the kinematic regime p T cut $$ {p}_T^{\textrm{cut}} $$ ≪ p T H $$ {p}_T^H $$ ∼ m H . We carry out the resummation at NNLL ′ accuracy, using theory nuisance parameters to account for the few unknown ingredients at this order, and match to full NNLO. We revisit the jet-veto factorization for this process and find that it requires refactorizing the total soft function into a global and soft-collinear contribution in order to fully account for logarithms of the signal jet radius. The leading nonglobal logarithms are also included, though they are numerically small for the region of phenomenological interest.https://doi.org/10.1007/JHEP03(2025)155FactorizationRenormalization GroupHiggs ProductionJets and Jet SubstructureResummation
spellingShingle Pedro Cal
Matthew A. Lim
Darren J. Scott
Frank J. Tackmann
Wouter J. Waalewijn
Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO
Journal of High Energy Physics
Factorization
Renormalization Group
Higgs Production
Jets and Jet Substructure
Resummation
title Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO
title_full Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO
title_fullStr Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO
title_full_unstemmed Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO
title_short Jet veto resummation for STXS H+1-jet bins at aNNLL′+NNLO
title_sort jet veto resummation for stxs h 1 jet bins at annll nnlo
topic Factorization
Renormalization Group
Higgs Production
Jets and Jet Substructure
Resummation
url https://doi.org/10.1007/JHEP03(2025)155
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AT darrenjscott jetvetoresummationforstxsh1jetbinsatannllnnlo
AT frankjtackmann jetvetoresummationforstxsh1jetbinsatannllnnlo
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