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WIMP and FIMP Dark Matter in Singlet-Triplet Fermionic Model
LAPTh, CNRS, USMB, 9 Chemin de Bellevue, 74940, Annecy, France, 9 Chemin de Bellevue.
KTH, School of Engineering Sciences (SCI), Physics, Particle and Astroparticle Physics.ORCID iD: 0000-0002-6071-8546
Centre for High Energy Physics, Indian Institute of Science, 560012, Bengaluru, India.
Institut für Theoretische Physik, Georg-August-Universität Göttingen, Friedrich-Hund-Platz 1, 37077, Göttingen, Germany, Friedrich-Hund-Platz 1.
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2024 (English)In: Proceedings of the XXV DAE-BRNS High Energy Physics (HEP) Symposium 2022, Springer Nature , 2024, p. 79-83Conference paper, Published paper (Refereed)
Abstract [en]

We present an extension of the SM involving three triplet fermions, one triplet scalar and one singlet fermion, which can explain both neutrino masses and dark matter. One triplet of fermions and the singlet are odd under a Z2 symmetry, thus the model features two possible dark matter candidates. The two remaining Z2-even triplet fermions can reproduce the neutrino masses and oscillation parameters consistent with observations. We consider the case where the singlet has feeble couplings while the triplet is weakly interacting and investigate the different possibilities for reproducing the observed dark matter relic density. This includes production of the triplet WIMP from freeze-out and from decay of the singlet as well as freeze-in production of the singlet from decay of particles that belong to the thermal bath or are thermally decoupled. While freeze-in production is usually dominated by decay processes, we also show cases where the annihilation of bath particles give substantial contribution to the final relic density. This occurs when the new scalars are below the TeV scale, thus in the reach of the LHC. The next-to-lightest odd particle can be long-lived and can alter the successful BBN predictions for the abundance of light elements, these constraints are relevant in both the scenarios where the singlet or the triplet are the long-lived particle.In the case where the triplet is the DM, the model is subject to constraints from ongoing direct, indirect and collider experiments. When the singlet is the DM, the triplet which is the next-to-lightest odd particle can be long-lived and can be probed at the proposed MATHUSLA detector. Finally we also address the detection prospects of triplet fermions and scalars at the LHC.

Place, publisher, year, edition, pages
Springer Nature , 2024. p. 79-83
National Category
Subatomic Physics
Identifiers
URN: urn:nbn:se:kth:diva-351949DOI: 10.1007/978-981-97-0289-3_16Scopus ID: 2-s2.0-85200500369OAI: oai:DiVA.org:kth-351949DiVA, id: diva2:1890165
Conference
25th DAE-BRNS High Energy Physics Symposium, HEPS 2022, IISER Mohali, India, Dec 12 2022 - Dec 16 2022
Note

Part of ISBN 9789819702886

QC 20240906

Available from: 2024-08-19 Created: 2024-08-19 Last updated: 2024-09-06Bibliographically approved

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Choubey, Sandhya

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