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Cosmological Implications of Dark Matter Bound States

We present generic formulæ for computing how Sommerfeld corrections together with bound-state formation affects the thermal abundance of Dark Matter with non-abelian gauge interactions. We consider DM as a fermion 3plet (wino) or 5plet under SU(2)L. In the latter case bound states raise to 11.5 TeV...

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Detalles Bibliográficos
Autores principales: Mitridate, Andrea, Redi, Michele, Smirnov, Juri, Strumia, Alessandro
Lenguaje:eng
Publicado: 2017
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1475-7516/2017/05/006
http://cds.cern.ch/record/2244886
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author Mitridate, Andrea
Redi, Michele
Smirnov, Juri
Strumia, Alessandro
author_facet Mitridate, Andrea
Redi, Michele
Smirnov, Juri
Strumia, Alessandro
author_sort Mitridate, Andrea
collection CERN
description We present generic formulæ for computing how Sommerfeld corrections together with bound-state formation affects the thermal abundance of Dark Matter with non-abelian gauge interactions. We consider DM as a fermion 3plet (wino) or 5plet under SU(2)L. In the latter case bound states raise to 11.5 TeV the DM mass required to reproduce the cosmological DM abundance and give indirect detection signals such as (for this mass) a dominant γ-line around 70 GeV. Furthermore, we consider DM co-annihilating with a colored particle, such as a squark or a gluino, finding that bound state effects are especially relevant in the latter case.
id cern-2244886
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2017
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spelling cern-22448862023-10-04T06:04:33Zdoi:10.1088/1475-7516/2017/05/006http://cds.cern.ch/record/2244886engMitridate, AndreaRedi, MicheleSmirnov, JuriStrumia, AlessandroCosmological Implications of Dark Matter Bound Stateshep-phParticle Physics - PhenomenologyWe present generic formulæ for computing how Sommerfeld corrections together with bound-state formation affects the thermal abundance of Dark Matter with non-abelian gauge interactions. We consider DM as a fermion 3plet (wino) or 5plet under SU(2)L. In the latter case bound states raise to 11.5 TeV the DM mass required to reproduce the cosmological DM abundance and give indirect detection signals such as (for this mass) a dominant γ-line around 70 GeV. Furthermore, we consider DM co-annihilating with a colored particle, such as a squark or a gluino, finding that bound state effects are especially relevant in the latter case.We present generic formulae for computing how Sommerfeld corrections together with bound-state formation affects the thermal abundance of Dark Matter with non-abelian gauge interactions. We consider DM as a fermion 3plet (wino) or 5plet under SU(2)$_L$. In the latter case bound states raise to 14 TeV the DM mass required to reproduce the cosmological DM abundance and give indirect detection signals such as (for this mass) a dominant $\gamma$-line around 85 GeV. Furthermore, we consider DM co-annihilating with a colored particle, such as a squark or a gluino, finding that bound state effects are especially relevant in the latter case.arXiv:1702.01141CERN-TH-2017-030IFUP-TH-2017oai:cds.cern.ch:22448862017-02-03
spellingShingle hep-ph
Particle Physics - Phenomenology
Mitridate, Andrea
Redi, Michele
Smirnov, Juri
Strumia, Alessandro
Cosmological Implications of Dark Matter Bound States
title Cosmological Implications of Dark Matter Bound States
title_full Cosmological Implications of Dark Matter Bound States
title_fullStr Cosmological Implications of Dark Matter Bound States
title_full_unstemmed Cosmological Implications of Dark Matter Bound States
title_short Cosmological Implications of Dark Matter Bound States
title_sort cosmological implications of dark matter bound states
topic hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1088/1475-7516/2017/05/006
http://cds.cern.ch/record/2244886
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AT redimichele cosmologicalimplicationsofdarkmatterboundstates
AT smirnovjuri cosmologicalimplicationsofdarkmatterboundstates
AT strumiaalessandro cosmologicalimplicationsofdarkmatterboundstates