Multipartite dark matter with scalars, fermions and signatures at LHC

Abstract Basic idea of this analysis is to achieve a two-component dark matter (DM) framework composed of a scalar and a fermion, with non-negligible DM-DM interaction contributing to thermal freeze out (hence relic density), but hiding them from direct detection bounds. We therefore augment the Sta...

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Published in:Journal of High Energy Physics
Main Authors: Subhaditya Bhattacharya, Purusottam Ghosh, Narendra Sahu
Format: Article
Language:English
Published: SpringerOpen 2019-02-01
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP02(2019)059
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author Subhaditya Bhattacharya
Purusottam Ghosh
Narendra Sahu
author_facet Subhaditya Bhattacharya
Purusottam Ghosh
Narendra Sahu
author_sort Subhaditya Bhattacharya
collection DOAJ
container_title Journal of High Energy Physics
description Abstract Basic idea of this analysis is to achieve a two-component dark matter (DM) framework composed of a scalar and a fermion, with non-negligible DM-DM interaction contributing to thermal freeze out (hence relic density), but hiding them from direct detection bounds. We therefore augment the Standard Model (SM) with a scalar singlet (S) and three vectorlike fermions: two singlets (χ 1 , χ 2) and a doublet (N). Stability of the two DM components is achieved by a discrete Z 2 × Z 2 ′ $$ {\mathcal{Z}}_2 \times {\mathcal{Z}}_2^{\prime } $$ symmetry, under which the additional fields transform suitably. Fermion fields having same Z 2 × Z 2 ′ $$ {\mathcal{Z}}_2 \times {\mathcal{Z}}_2^{\prime } $$ charge (N, χ 1 in the model) mix after electroweak symmetry breaking (EWSB) and the lightest component becomes one of the DM candidates, while scalar singlet S is the other DM component connected to visible sector by Higgs portal coupling. The heavy fermion (χ 2) plays the role of mediator to connect the two DM candidates through Yukawa interaction. This opens up a large parameter space for the heavier DM component through DM-DM conversion. Hadronically quiet dilepton signature, arising from the fermion dark sector, can be observed at Large Hadron Collider (LHC) aided by the presence of a lighter scalar DM component, satisfying relic density and direct search bounds through DM-DM conversion.
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spelling doaj-art-4a382b46c53b4cccbbb8a88e5016ba502025-08-19T21:13:00ZengSpringerOpenJournal of High Energy Physics1029-84792019-02-012019214410.1007/JHEP02(2019)059Multipartite dark matter with scalars, fermions and signatures at LHCSubhaditya Bhattacharya0Purusottam Ghosh1Narendra Sahu2Department of Physics, Indian Institute of Technology GuwahatiDepartment of Physics, Indian Institute of Technology GuwahatiDepartment of Physics, Indian Institute of Technology HyderabadAbstract Basic idea of this analysis is to achieve a two-component dark matter (DM) framework composed of a scalar and a fermion, with non-negligible DM-DM interaction contributing to thermal freeze out (hence relic density), but hiding them from direct detection bounds. We therefore augment the Standard Model (SM) with a scalar singlet (S) and three vectorlike fermions: two singlets (χ 1 , χ 2) and a doublet (N). Stability of the two DM components is achieved by a discrete Z 2 × Z 2 ′ $$ {\mathcal{Z}}_2 \times {\mathcal{Z}}_2^{\prime } $$ symmetry, under which the additional fields transform suitably. Fermion fields having same Z 2 × Z 2 ′ $$ {\mathcal{Z}}_2 \times {\mathcal{Z}}_2^{\prime } $$ charge (N, χ 1 in the model) mix after electroweak symmetry breaking (EWSB) and the lightest component becomes one of the DM candidates, while scalar singlet S is the other DM component connected to visible sector by Higgs portal coupling. The heavy fermion (χ 2) plays the role of mediator to connect the two DM candidates through Yukawa interaction. This opens up a large parameter space for the heavier DM component through DM-DM conversion. Hadronically quiet dilepton signature, arising from the fermion dark sector, can be observed at Large Hadron Collider (LHC) aided by the presence of a lighter scalar DM component, satisfying relic density and direct search bounds through DM-DM conversion.http://link.springer.com/article/10.1007/JHEP02(2019)059Beyond Standard ModelCosmology of Theories beyond the SM
spellingShingle Subhaditya Bhattacharya
Purusottam Ghosh
Narendra Sahu
Multipartite dark matter with scalars, fermions and signatures at LHC
Beyond Standard Model
Cosmology of Theories beyond the SM
title Multipartite dark matter with scalars, fermions and signatures at LHC
title_full Multipartite dark matter with scalars, fermions and signatures at LHC
title_fullStr Multipartite dark matter with scalars, fermions and signatures at LHC
title_full_unstemmed Multipartite dark matter with scalars, fermions and signatures at LHC
title_short Multipartite dark matter with scalars, fermions and signatures at LHC
title_sort multipartite dark matter with scalars fermions and signatures at lhc
topic Beyond Standard Model
Cosmology of Theories beyond the SM
url http://link.springer.com/article/10.1007/JHEP02(2019)059
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AT purusottamghosh multipartitedarkmatterwithscalarsfermionsandsignaturesatlhc
AT narendrasahu multipartitedarkmatterwithscalarsfermionsandsignaturesatlhc