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Colored Dark Matter

We explore the possibility that dark matter (DM) is the lightest hadron made of two stable color octet Dirac fermions Q. The cosmological DM abundance is reproduced for MQ≈12.5  TeV, compatibly with direct searches (the Rayleigh cross section, suppressed by 1/MQ6, is close to present bounds), indire...

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Detalles Bibliográficos
Autores principales: De Luca, Valerio, Mitridate, Andrea, Redi, Michele, Smirnov, Juri, Strumia, Alessandro
Lenguaje:eng
Publicado: 2018
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.97.115024
http://cds.cern.ch/record/2299437
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author De Luca, Valerio
Mitridate, Andrea
Redi, Michele
Smirnov, Juri
Strumia, Alessandro
author_facet De Luca, Valerio
Mitridate, Andrea
Redi, Michele
Smirnov, Juri
Strumia, Alessandro
author_sort De Luca, Valerio
collection CERN
description We explore the possibility that dark matter (DM) is the lightest hadron made of two stable color octet Dirac fermions Q. The cosmological DM abundance is reproduced for MQ≈12.5  TeV, compatibly with direct searches (the Rayleigh cross section, suppressed by 1/MQ6, is close to present bounds), indirect searches (enhanced by QQ+Q¯Q¯→QQ¯+QQ¯ recombination), and with collider searches (where Q manifests as tracks, pair produced via QCD). Hybrid hadrons, made of Q and of standard model quarks and gluons, have large QCD cross sections, and do not reach underground detectors. Their cosmological abundance is 105 times smaller than DM, such that their unusual signals seem compatible with bounds. Those in the Earth and stars sank to their centers; the Earth crust and meteorites later accumulate a secondary abundance, although their present abundance depends on nuclear and geological properties that we cannot compute from first principles.
id cern-2299437
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2018
record_format invenio
spelling cern-22994372023-07-11T04:15:15Zdoi:10.1103/PhysRevD.97.115024http://cds.cern.ch/record/2299437engDe Luca, ValerioMitridate, AndreaRedi, MicheleSmirnov, JuriStrumia, AlessandroColored Dark Matternucl-thNuclear Physics - Theoryastro-ph.COAstrophysics and Astronomyhep-phParticle Physics - PhenomenologyWe explore the possibility that dark matter (DM) is the lightest hadron made of two stable color octet Dirac fermions Q. The cosmological DM abundance is reproduced for MQ≈12.5  TeV, compatibly with direct searches (the Rayleigh cross section, suppressed by 1/MQ6, is close to present bounds), indirect searches (enhanced by QQ+Q¯Q¯→QQ¯+QQ¯ recombination), and with collider searches (where Q manifests as tracks, pair produced via QCD). Hybrid hadrons, made of Q and of standard model quarks and gluons, have large QCD cross sections, and do not reach underground detectors. Their cosmological abundance is 105 times smaller than DM, such that their unusual signals seem compatible with bounds. Those in the Earth and stars sank to their centers; the Earth crust and meteorites later accumulate a secondary abundance, although their present abundance depends on nuclear and geological properties that we cannot compute from first principles.We explore the possibility that Dark Matter is the lightest hadron made of two stable color octet Dirac fermions ${\cal Q}$. The cosmological DM abundance is reproduced for $M_{\cal Q}\approx 12.5$ TeV, compatibly with direct searches (the Rayleigh cross section, suppressed by $1/M_{\cal Q}^6$, is close to present bounds), indirect searches (enhanced by ${\cal Q}{\cal Q}+\bar{\cal Q}\bar{\cal Q}\to {\cal Q}\bar{\cal Q}+{\cal Q}\bar{\cal Q}$ recombination), and with collider searches (where ${\cal Q}$ manifests as tracks, pair produced via QCD). Hybrid hadrons, made of $\cal Q$ and of SM quarks and gluons, have large QCD cross sections, and do not reach underground detectors. Their cosmological abundance is $10^5$ times smaller than DM, such that their unusual signals seem compatible with bounds. Those in the Earth and stars sank to their centers; the Earth crust and meteorites later accumulate a secondary abundance, although their present abundance depends on nuclear and geological properties that we cannot compute from first principles.arXiv:1801.01135IFUP-TH-2017CERN-TH-2017-283IFUP-TH/2017oai:cds.cern.ch:22994372018-01-03
spellingShingle nucl-th
Nuclear Physics - Theory
astro-ph.CO
Astrophysics and Astronomy
hep-ph
Particle Physics - Phenomenology
De Luca, Valerio
Mitridate, Andrea
Redi, Michele
Smirnov, Juri
Strumia, Alessandro
Colored Dark Matter
title Colored Dark Matter
title_full Colored Dark Matter
title_fullStr Colored Dark Matter
title_full_unstemmed Colored Dark Matter
title_short Colored Dark Matter
title_sort colored dark matter
topic nucl-th
Nuclear Physics - Theory
astro-ph.CO
Astrophysics and Astronomy
hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.97.115024
http://cds.cern.ch/record/2299437
work_keys_str_mv AT delucavalerio coloreddarkmatter
AT mitridateandrea coloreddarkmatter
AT redimichele coloreddarkmatter
AT smirnovjuri coloreddarkmatter
AT strumiaalessandro coloreddarkmatter