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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>&...
Autores principales: | , , , , |
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Lenguaje: | eng |
Publicado: |
2023
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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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