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Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach
We study dark matter freeze-in scenarios where the mass of the mediator particle that couples dark matter to the Standard Model is larger than the reheat temperature, T$_{RH}$, in the early Universe. In such setups, the standard approach is to work with an effective field theory (EFT) where the medi...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2021
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP09(2022)083 http://cds.cern.ch/record/2788513 |
_version_ | 1780972134582976512 |
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author | Frangipane, Evan Gori, Stefania Shakya, Bibhushan |
author_facet | Frangipane, Evan Gori, Stefania Shakya, Bibhushan |
author_sort | Frangipane, Evan |
collection | CERN |
description | We study dark matter freeze-in scenarios where the mass of the mediator particle that couples dark matter to the Standard Model is larger than the reheat temperature, T$_{RH}$, in the early Universe. In such setups, the standard approach is to work with an effective field theory (EFT) where the mediator is integrated out. We examine the validity of this approach in various generic s- and t-channel mediator frameworks. We find that the EFT approach breaks down when the mediator mass is between one to two orders of magnitude larger than T$_{RH}$ due to various effects such as s-channel resonance, a small thermally-suppressed abundance of the mediator, or decays of Standard Model particles through loops induced by the mediator. This highlights the necessity of including these contributions in such dark matter freeze-in studies. We also discuss the collider phenomenology of the heavy mediators, which is qualitatively different from standard freeze-in scenarios. We highlight that, due to the low T$_{RH}$, the Standard Model-dark matter coupling in these scenarios can be relatively larger than in standard freeze-in scenarios, improving the testability prospects of these setups. |
id | cern-2788513 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2021 |
record_format | invenio |
spelling | cern-27885132023-02-02T15:18:21Zdoi:10.1007/JHEP09(2022)083http://cds.cern.ch/record/2788513engFrangipane, EvanGori, StefaniaShakya, BibhushanDark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approachhep-phParticle Physics - PhenomenologyWe study dark matter freeze-in scenarios where the mass of the mediator particle that couples dark matter to the Standard Model is larger than the reheat temperature, T$_{RH}$, in the early Universe. In such setups, the standard approach is to work with an effective field theory (EFT) where the mediator is integrated out. We examine the validity of this approach in various generic s- and t-channel mediator frameworks. We find that the EFT approach breaks down when the mediator mass is between one to two orders of magnitude larger than T$_{RH}$ due to various effects such as s-channel resonance, a small thermally-suppressed abundance of the mediator, or decays of Standard Model particles through loops induced by the mediator. This highlights the necessity of including these contributions in such dark matter freeze-in studies. We also discuss the collider phenomenology of the heavy mediators, which is qualitatively different from standard freeze-in scenarios. We highlight that, due to the low T$_{RH}$, the Standard Model-dark matter coupling in these scenarios can be relatively larger than in standard freeze-in scenarios, improving the testability prospects of these setups.We study dark matter freeze-in scenarios where the mass of the mediator particle that couples dark matter to the Standard Model is larger than the reheat temperature, TRH, in the early Universe. In such setups, the standard approach is to work with an effective field theory (EFT) where the mediator is integrated out. We examine the validity of this approach in various generic s- and t-channel mediator frameworks. We find that the EFT approach breaks down when the mediator mass is between one to two orders of magnitude larger than TRH due to various effects such as s-channel resonance, a small thermally-suppressed abundance of the mediator, or decays of Standard Model particles through loops induced by the mediator. This highlights the necessity of including these contributions in such dark matter freeze-in studies. We also discuss the collider phenomenology of the heavy mediators, which is qualitatively different from standard freeze-in scenarios. We highlight that, due to the low TRH, the Standard Model-dark matter coupling in these scenarios can be relatively larger than in standard freeze-in scenarios, improving the testability prospects of these setups.arXiv:2110.10711CERN-TH-2021-120DESY-21-117oai:cds.cern.ch:27885132021-10-20 |
spellingShingle | hep-ph Particle Physics - Phenomenology Frangipane, Evan Gori, Stefania Shakya, Bibhushan Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach |
title | Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach |
title_full | Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach |
title_fullStr | Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach |
title_full_unstemmed | Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach |
title_short | Dark Matter Freeze-In with a Heavy Mediator: Beyond the EFT Approach |
title_sort | dark matter freeze-in with a heavy mediator: beyond the eft approach |
topic | hep-ph Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1007/JHEP09(2022)083 http://cds.cern.ch/record/2788513 |
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