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C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling

Higgs pair production processes provide the direct probe to the Higgs boson self-coupling ($\lambda_{3}$). However, as well known such a processes have a small production cross section. It is also known that single Higgs processes indirectly depends on $\lambda_{3}$, thus an alternative method to me...

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Detalles Bibliográficos
Autores principales: Lucio Alves, Fabio Lucio, ATLAS Collaboration
Lenguaje:eng
Publicado: 2023
Materias:
Acceso en línea:http://cds.cern.ch/record/2871454
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author Lucio Alves, Fabio Lucio
ATLAS Collaboration
author_facet Lucio Alves, Fabio Lucio
ATLAS Collaboration
author_sort Lucio Alves, Fabio Lucio
collection CERN
description Higgs pair production processes provide the direct probe to the Higgs boson self-coupling ($\lambda_{3}$). However, as well known such a processes have a small production cross section. It is also known that single Higgs processes indirectly depends on $\lambda_{3}$, thus an alternative method to measure the $\lambda_{3}$ is considering $\lambda_{3}$-dependent NLO EW corrections in single Higgs processes. The magnitude of these corrections are encoded by some process and kinematic-dependent coefficients named as C1. In the following, an overview of the parametrization of the C1 coefficients and K-factors in STXS bins performed by ATLAS and CMS are shown.
id cern-2871454
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2023
record_format invenio
spelling cern-28714542023-09-16T18:53:51Zhttp://cds.cern.ch/record/2871454engLucio Alves, Fabio LucioATLAS CollaborationC1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-couplingParticle Physics - ExperimentHiggs pair production processes provide the direct probe to the Higgs boson self-coupling ($\lambda_{3}$). However, as well known such a processes have a small production cross section. It is also known that single Higgs processes indirectly depends on $\lambda_{3}$, thus an alternative method to measure the $\lambda_{3}$ is considering $\lambda_{3}$-dependent NLO EW corrections in single Higgs processes. The magnitude of these corrections are encoded by some process and kinematic-dependent coefficients named as C1. In the following, an overview of the parametrization of the C1 coefficients and K-factors in STXS bins performed by ATLAS and CMS are shown.ATL-PHYS-SLIDE-2023-444oai:cds.cern.ch:28714542023-09-16
spellingShingle Particle Physics - Experiment
Lucio Alves, Fabio Lucio
ATLAS Collaboration
C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling
title C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling
title_full C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling
title_fullStr C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling
title_full_unstemmed C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling
title_short C1 and $K_{EW}$ factors parametrization in STXS bins for constraining the Higgs boson self-coupling
title_sort c1 and $k_{ew}$ factors parametrization in stxs bins for constraining the higgs boson self-coupling
topic Particle Physics - Experiment
url http://cds.cern.ch/record/2871454
work_keys_str_mv AT lucioalvesfabiolucio c1andkewfactorsparametrizationinstxsbinsforconstrainingthehiggsbosonselfcoupling
AT atlascollaboration c1andkewfactorsparametrizationinstxsbinsforconstrainingthehiggsbosonselfcoupling