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A seesaw model for large neutrino masses in concordance with cosmology

Cosmological constraints on the sum of the neutrino masses can be relaxed if the number density of active neutrinos is reduced compared to the standard scenario, while at the same time keeping the effective number of neutrino species N$_{eff}$ ≈ 3 by introducing a new component of dark radiation. We...

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Detalles Bibliográficos
Autores principales: Escudero, Miguel, Schwetz, Thomas, Terol-Calvo, Jorge
Lenguaje:eng
Publicado: 2022
Materias:
Acceso en línea:https://dx.doi.org/10.1007/JHEP02(2023)142
http://cds.cern.ch/record/2839588
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author Escudero, Miguel
Schwetz, Thomas
Terol-Calvo, Jorge
author_facet Escudero, Miguel
Schwetz, Thomas
Terol-Calvo, Jorge
author_sort Escudero, Miguel
collection CERN
description Cosmological constraints on the sum of the neutrino masses can be relaxed if the number density of active neutrinos is reduced compared to the standard scenario, while at the same time keeping the effective number of neutrino species N$_{eff}$ ≈ 3 by introducing a new component of dark radiation. We discuss a UV complete model to realise this idea, which simultaneously provides neutrino masses via the seesaw mechanism. It is based on a U(1) symmetry in the dark sector, which can be either gauged or global. In addition to heavy seesaw neutrinos, we need to introduce 𝒪(10) generations of massless sterile neutrinos providing the dark radiation. Then we can accommodate active neutrino masses with ∑m$_{ν}$ ~ 1 eV, in the sensitivity range of the KATRIN experiment. We discuss the phenomenology of the model and identify the allowed parameter space. We argue that the gauged version of the model is preferred, and in this case the typical energy scale of the model is in the 10 MeV to few GeV range.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2022
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spelling cern-28395882023-05-07T02:34:13Zdoi:10.1007/JHEP02(2023)142http://cds.cern.ch/record/2839588engEscudero, MiguelSchwetz, ThomasTerol-Calvo, JorgeA seesaw model for large neutrino masses in concordance with cosmologyastro-ph.COAstrophysics and Astronomyhep-phParticle Physics - PhenomenologyCosmological constraints on the sum of the neutrino masses can be relaxed if the number density of active neutrinos is reduced compared to the standard scenario, while at the same time keeping the effective number of neutrino species N$_{eff}$ ≈ 3 by introducing a new component of dark radiation. We discuss a UV complete model to realise this idea, which simultaneously provides neutrino masses via the seesaw mechanism. It is based on a U(1) symmetry in the dark sector, which can be either gauged or global. In addition to heavy seesaw neutrinos, we need to introduce 𝒪(10) generations of massless sterile neutrinos providing the dark radiation. Then we can accommodate active neutrino masses with ∑m$_{ν}$ ~ 1 eV, in the sensitivity range of the KATRIN experiment. We discuss the phenomenology of the model and identify the allowed parameter space. We argue that the gauged version of the model is preferred, and in this case the typical energy scale of the model is in the 10 MeV to few GeV range.Cosmological constraints on the sum of the neutrino masses can be relaxed if the number density of active neutrinos is reduced compared to the standard scenario, while at the same time keeping the effective number of neutrino species $N_{\rm eff}\approx 3$ by introducing a new component of dark radiation. We discuss a UV complete model to realise this idea, which simultaneously provides neutrino masses via the seesaw mechanism. It is based on a $U(1)$ symmetry in the dark sector, which can be either gauged or global. In addition to heavy seesaw neutrinos, we need to introduce $\mathcal{O}(10)$ generations of massless sterile neutrinos providing the dark radiation. Then we can accommodate active neutrino masses with $\sum m_\nu \sim 1$ eV, in the sensitivity range of the KATRIN experiment. We discuss the phenomenology of the model and identify the allowed parameter space. We argue that the gauged version of the model is preferred, and in this case the typical energy scale of the model is in the 10 MeV to few GeV range.arXiv:2211.01729CERN-TH-2022-180oai:cds.cern.ch:28395882022-11-03
spellingShingle astro-ph.CO
Astrophysics and Astronomy
hep-ph
Particle Physics - Phenomenology
Escudero, Miguel
Schwetz, Thomas
Terol-Calvo, Jorge
A seesaw model for large neutrino masses in concordance with cosmology
title A seesaw model for large neutrino masses in concordance with cosmology
title_full A seesaw model for large neutrino masses in concordance with cosmology
title_fullStr A seesaw model for large neutrino masses in concordance with cosmology
title_full_unstemmed A seesaw model for large neutrino masses in concordance with cosmology
title_short A seesaw model for large neutrino masses in concordance with cosmology
title_sort seesaw model for large neutrino masses in concordance with cosmology
topic astro-ph.CO
Astrophysics and Astronomy
hep-ph
Particle Physics - Phenomenology
url https://dx.doi.org/10.1007/JHEP02(2023)142
http://cds.cern.ch/record/2839588
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AT terolcalvojorge aseesawmodelforlargeneutrinomassesinconcordancewithcosmology
AT escuderomiguel seesawmodelforlargeneutrinomassesinconcordancewithcosmology
AT schwetzthomas seesawmodelforlargeneutrinomassesinconcordancewithcosmology
AT terolcalvojorge seesawmodelforlargeneutrinomassesinconcordancewithcosmology