Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry
Abstract We study dark matter (DM) abundance in the framework of the extension of the Standard Model (SM) with an additional $$U(1)_X$$ U(1)X gauge symmetry. One complex singlet is included to break the $$U(1)_X$$ U(1)X gauge symmetry, meanwhile one of the doublets is considered inert to introduce a...
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doaj-cccbd1da38284996ab57b2f0927975882020-11-25T03:48:49ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522020-08-0180811410.1140/epjc/s10052-020-8316-9Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetryM. A. Arroyo-Ureña0R. Gaitan1R. Martinez2J. H. Montes de Oca Yemha3Departamento de Física, FES-Cuautitlán, Universidad Nacional Autónoma de MéxicoDepartamento de Física, FES-Cuautitlán, Universidad Nacional Autónoma de MéxicoDepartamento de Física, Universidad Nacional de ColombiaDepartamento de Física, FES-Cuautitlán, Universidad Nacional Autónoma de MéxicoAbstract We study dark matter (DM) abundance in the framework of the extension of the Standard Model (SM) with an additional $$U(1)_X$$ U(1)X gauge symmetry. One complex singlet is included to break the $$U(1)_X$$ U(1)X gauge symmetry, meanwhile one of the doublets is considered inert to introduce a DM candidate. The stability of the DM candidate is analyzed with a continuous $$U(1)_X$$ U(1)X gauge symmetry as well as discrete $$Z_2$$ Z2 symmetry. We find allowed regions for the free model parameters which are in agreement with the most up-to-date experimental results reported by CMS and ATLAS Collaborations, the upper limit on WIMP-nucleon cross section imposed by XENON1T Collaboration and the upper limit on the production cross-section of a $$Z^{\prime }$$ Z′ gauge boson times the branching ratio of the $$Z^{\prime }$$ Z′ boson decaying into $$\ell ^-\ell ^+$$ ℓ-ℓ+ . We also obtain allowed regions for the DM candidate mass from the relic density reported by the PLANCK Collaboration including light, intermediate and heavy masses; depending mainly on two parameters of the scalar potential, $$\lambda _{2x}$$ λ2x and $$\lambda _{345}=\lambda _3+\lambda _4+2\lambda _5$$ λ345=λ3+λ4+2λ5 . We find that trough $$pp\rightarrow \chi \chi \gamma $$ pp→χχγ production, it may only be possible for a future hadron–hadron circular collider (FCC-hh) to be able to detect a DM candidate within the range of masses 10–60 GeV.http://link.springer.com/article/10.1140/epjc/s10052-020-8316-9 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
M. A. Arroyo-Ureña R. Gaitan R. Martinez J. H. Montes de Oca Yemha |
spellingShingle |
M. A. Arroyo-Ureña R. Gaitan R. Martinez J. H. Montes de Oca Yemha Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry European Physical Journal C: Particles and Fields |
author_facet |
M. A. Arroyo-Ureña R. Gaitan R. Martinez J. H. Montes de Oca Yemha |
author_sort |
M. A. Arroyo-Ureña |
title |
Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry |
title_short |
Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry |
title_full |
Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry |
title_fullStr |
Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry |
title_full_unstemmed |
Dark matter in inert doublet model with one scalar singlet and $$U(1)_X$$ U(1)X gauge symmetry |
title_sort |
dark matter in inert doublet model with one scalar singlet and $$u(1)_x$$ u(1)x gauge symmetry |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2020-08-01 |
description |
Abstract We study dark matter (DM) abundance in the framework of the extension of the Standard Model (SM) with an additional $$U(1)_X$$ U(1)X gauge symmetry. One complex singlet is included to break the $$U(1)_X$$ U(1)X gauge symmetry, meanwhile one of the doublets is considered inert to introduce a DM candidate. The stability of the DM candidate is analyzed with a continuous $$U(1)_X$$ U(1)X gauge symmetry as well as discrete $$Z_2$$ Z2 symmetry. We find allowed regions for the free model parameters which are in agreement with the most up-to-date experimental results reported by CMS and ATLAS Collaborations, the upper limit on WIMP-nucleon cross section imposed by XENON1T Collaboration and the upper limit on the production cross-section of a $$Z^{\prime }$$ Z′ gauge boson times the branching ratio of the $$Z^{\prime }$$ Z′ boson decaying into $$\ell ^-\ell ^+$$ ℓ-ℓ+ . We also obtain allowed regions for the DM candidate mass from the relic density reported by the PLANCK Collaboration including light, intermediate and heavy masses; depending mainly on two parameters of the scalar potential, $$\lambda _{2x}$$ λ2x and $$\lambda _{345}=\lambda _3+\lambda _4+2\lambda _5$$ λ345=λ3+λ4+2λ5 . We find that trough $$pp\rightarrow \chi \chi \gamma $$ pp→χχγ production, it may only be possible for a future hadron–hadron circular collider (FCC-hh) to be able to detect a DM candidate within the range of masses 10–60 GeV. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-020-8316-9 |
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