Heavy neutrino as dark matter in a neutrinophilic U(1) model

Abstract We study the prospect of heavy singlet neutrinos as a dark matter (DM) candidate within a neutrinophilic U (1) model, where the Standard Model (SM) is extended with a U (1) gauge symmetry, and neutrino mass and oscillation parameters are explained through an inverse see-saw mechanism. The lightest of the heavy neutrinos plays the role of the DM, while the newly introduced scalars and the extra gauge boson $$Z'$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>Z</mml:mi> <mml:mo>′</mml:mo> </mml:msup> </mml:math> act as mediators between the dark sector and the SM sector. We show the range of model parameters where this DM candidate can be accommodated in the Weakly Interacting Massive Particle (WIMP) or Feebly Interacting Massive Particle (FIMP) scenario. The observed DM relic density (DMRD) is achieved via the new gauge boson and singlet scalar portals in the WIMP scenario, whereas within the FIMP scenario, these two particles assume a distinct yet pivotal role in generating the observed DMRD.

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Publication Details

Journal
The European Physical Journal C
Published
2024-10-19
DOI
https://doi.org/10.1140/epjc/s10052-024-13407-z
Citations
2
Primary Topic
Particle physics theoretical and experimental studies
Type
article
Field-Weighted Citation Impact
1.32
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article

Heavy neutrino as dark matter in a neutrinophilic U(1) model

Tousik Samui, Anjan Kumar Barik, Waleed Abdallah, Santosh Kumar
2 citations
The European Physical Journal C
Particle physics theoretical and experimental studies
1.32
article

Heavy neutrino as dark matter in a neutrinophilic U(1) model

Tousik Samui, Anjan Kumar Barik, Waleed Abdallah, Santosh Kumar
article en
2 citations

Abstract

Abstract We study the prospect of heavy singlet neutrinos as a dark matter (DM) candidate within a neutrinophilic U (1) model, where the Standard Model (SM) is extended with a U (1) gauge symmetry, and neutrino mass and oscillation parameters are explained through an inverse see-saw mechanism. The lightest of the heavy neutrinos plays the role of the DM, while the newly introduced scalars and the extra gauge boson $$Z'$$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup> <mml:mi>Z</mml:mi> <mml:mo>′</mml:mo> </mml:msup> </mml:math> act as mediators between the dark sector and the SM sector. We show the range of model parameters where this DM candidate can be accommodated in the Weakly Interacting Massive Particle (WIMP) or Feebly Interacting Massive Particle (FIMP) scenario. The observed DM relic density (DMRD) is achieved via the new gauge boson and singlet scalar portals in the WIMP scenario, whereas within the FIMP scenario, these two particles assume a distinct yet pivotal role in generating the observed DMRD.

The European Physical Journal CVol. 84(10)
Indian Institute of Science Education and Research Kolkata (IN), Cairo University (EG), Homi Bhabha National Institute (IN), Harish-Chandra Research Institute (IN), Institute of Mathematical Sciences (IN)
Openalex Percentile: Top 11%
Particle physics theoretical and experimental studies
1.32
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Heavy neutrino as dark matter in a neutrinophilic U(1) model — Tousik Samui, Anjan Kumar Barik, et al. · The European Physical Journal C (2024) | TGRS Research Map | TGRS