Cargando…
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...
Autores principales: | , , |
---|---|
Lenguaje: | eng |
Publicado: |
2022
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1007/JHEP02(2023)142 http://cds.cern.ch/record/2839588 |
_version_ | 1780975973525618688 |
---|---|
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. |
id | cern-2839588 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2022 |
record_format | invenio |
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 |
work_keys_str_mv | AT escuderomiguel aseesawmodelforlargeneutrinomassesinconcordancewithcosmology AT schwetzthomas aseesawmodelforlargeneutrinomassesinconcordancewithcosmology AT terolcalvojorge aseesawmodelforlargeneutrinomassesinconcordancewithcosmology AT escuderomiguel seesawmodelforlargeneutrinomassesinconcordancewithcosmology AT schwetzthomas seesawmodelforlargeneutrinomassesinconcordancewithcosmology AT terolcalvojorge seesawmodelforlargeneutrinomassesinconcordancewithcosmology |