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Collider constraints on massive gravitons coupling to photons

We study the discovery potential of massive graviton-like spin-2 particles coupled to standard model fields, produced in photon-photon collisions at the Large Hadron Collider (LHC) as well as in electron-positron (<math altimg="si1.svg"><msup><mrow><mi>e</mi>&...

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Detalles Bibliográficos
Autores principales: d'Enterria, David, Tamlihat, Malak Ait, Schoeffel, Laurent, Shao, Hua-Sheng, Tayalati, Yahya
Lenguaje:eng
Publicado: 2023
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.physletb.2023.138237
http://cds.cern.ch/record/2864939
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author d'Enterria, David
Tamlihat, Malak Ait
Schoeffel, Laurent
Shao, Hua-Sheng
Tayalati, Yahya
author_facet d'Enterria, David
Tamlihat, Malak Ait
Schoeffel, Laurent
Shao, Hua-Sheng
Tayalati, Yahya
author_sort d'Enterria, David
collection CERN
description We study the discovery potential of massive graviton-like spin-2 particles coupled to standard model fields, produced in photon-photon collisions at the Large Hadron Collider (LHC) as well as in electron-positron (<math altimg="si1.svg"><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo></mrow></msup></math>) collisions, within an effective theory with and without universal couplings. Our focus is on a massive graviton G coupled to the electromagnetic field, which decays via <math altimg="si2.svg"><mi mathvariant="normal">G</mi><mo stretchy="false">→</mo><mi>γ</mi><mi>γ</mi></math> and leads to a resonant excess of diphotons over the light-by-light scattering continuum at the LHC, and of triphoton final states at <math altimg="si1.svg"><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo></mrow></msup></math> colliders. Based on similar searches performed for pseudoscalar axion-like particles (ALPs), and taking into account the different cross sections, γγ partial widths, and decay kinematics of the pseudoscalar and tensor particles, we reinterpret existing experimental bounds on the ALP-γ coupling into G-γ ones. Using the available data, exclusion limits on the graviton-photon coupling are set down to <math altimg="si154.svg"><msub><mrow><mi>g</mi></mrow><mrow><mi mathvariant="normal">G</mi><mi>γ</mi></mrow></msub><mo>≈</mo><mn>1</mn></math>–0.05 TeV<sup loc="post">−1</sup> for masses <math altimg="si4.svg"><msub><mrow><mi>m</mi></mrow><mrow><mi mathvariant="normal">G</mi></mrow></msub><mo>≈</mo><mn>100</mn></math> MeV–2 TeV. Such bounds can be improved by factors of 100 at Belle II in the low-mass region, and of 4 at the HL-LHC at high masses, with their expected full integrated luminosities.
id cern-2864939
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2023
record_format invenio
spelling cern-28649392023-10-19T02:16:04Zdoi:10.1016/j.physletb.2023.138237http://cds.cern.ch/record/2864939engd'Enterria, DavidTamlihat, Malak AitSchoeffel, LaurentShao, Hua-ShengTayalati, YahyaCollider constraints on massive gravitons coupling to photonsnucl-thNuclear Physics - Theorynucl-exNuclear Physics - Experimenthep-exParticle Physics - Experimenthep-phParticle Physics - PhenomenologyWe study the discovery potential of massive graviton-like spin-2 particles coupled to standard model fields, produced in photon-photon collisions at the Large Hadron Collider (LHC) as well as in electron-positron (<math altimg="si1.svg"><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo></mrow></msup></math>) collisions, within an effective theory with and without universal couplings. Our focus is on a massive graviton G coupled to the electromagnetic field, which decays via <math altimg="si2.svg"><mi mathvariant="normal">G</mi><mo stretchy="false">→</mo><mi>γ</mi><mi>γ</mi></math> and leads to a resonant excess of diphotons over the light-by-light scattering continuum at the LHC, and of triphoton final states at <math altimg="si1.svg"><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">+</mo></mrow></msup><msup><mrow><mi>e</mi></mrow><mrow><mo linebreak="badbreak" linebreakstyle="after">−</mo></mrow></msup></math> colliders. Based on similar searches performed for pseudoscalar axion-like particles (ALPs), and taking into account the different cross sections, γγ partial widths, and decay kinematics of the pseudoscalar and tensor particles, we reinterpret existing experimental bounds on the ALP-γ coupling into G-γ ones. Using the available data, exclusion limits on the graviton-photon coupling are set down to <math altimg="si154.svg"><msub><mrow><mi>g</mi></mrow><mrow><mi mathvariant="normal">G</mi><mi>γ</mi></mrow></msub><mo>≈</mo><mn>1</mn></math>–0.05 TeV<sup loc="post">−1</sup> for masses <math altimg="si4.svg"><msub><mrow><mi>m</mi></mrow><mrow><mi mathvariant="normal">G</mi></mrow></msub><mo>≈</mo><mn>100</mn></math> MeV–2 TeV. Such bounds can be improved by factors of 100 at Belle II in the low-mass region, and of 4 at the HL-LHC at high masses, with their expected full integrated luminosities.We study the discovery potential of massive graviton-like spin-2 particles coupled to standard model fields, produced in photon-photon collisions at the Large Hadron Collider (LHC) as well as in electron-positron ($e^+e^-$) collisions, within an effective theory with and without universal couplings. Our focus is on a massive graviton G coupled to the electromagnetic field, which decays via $\mathrm{G}\to \gamma \gamma$ and leads to a resonant excess of diphotons over the light-by-light scattering continuum at the LHC, and of triphoton final states at $e^+e^-$ colliders. Based on similar searches performed for pseudoscalar axion-like particles (ALPs), and taking into account the different cross sections, $\gamma \gamma$ partial widths, and decay kinematics of the pseudoscalar and tensor particles, we reinterpret existing experimental bounds on the ALP-$\gamma$ coupling into G-$\gamma$ ones. Using the available data, exclusion limits on the graviton-photon coupling are set down to $g_{\mathrm{G}\gamma\gamma}\approx 1$--0.05~TeV$^{-1}$ for masses $m_\mathrm{G} \approx 100$~MeV--2~TeV. Such bounds can be improved by factors of 100 at Belle~II in the low-mass region, and of 4 at the HL-LHC at high masses, with their expected full integrated luminosities.arXiv:2306.15558oai:cds.cern.ch:28649392023-06-27
spellingShingle nucl-th
Nuclear Physics - Theory
nucl-ex
Nuclear Physics - Experiment
hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
d'Enterria, David
Tamlihat, Malak Ait
Schoeffel, Laurent
Shao, Hua-Sheng
Tayalati, Yahya
Collider constraints on massive gravitons coupling to photons
title Collider constraints on massive gravitons coupling to photons
title_full Collider constraints on massive gravitons coupling to photons
title_fullStr Collider constraints on massive gravitons coupling to photons
title_full_unstemmed Collider constraints on massive gravitons coupling to photons
title_short Collider constraints on massive gravitons coupling to photons
title_sort collider constraints on massive gravitons coupling to photons
topic nucl-th
Nuclear Physics - Theory
nucl-ex
Nuclear Physics - Experiment
hep-ex
Particle Physics - Experiment
hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.physletb.2023.138237
http://cds.cern.ch/record/2864939
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