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Related papers: Singlet Fermionic Dark Matter with Dark $Z$

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We consider $U(1)_H$ extensions of Type-I 2HDM plus a singlet scalar $\phi_H$, introducing a new Higgs doublet $H_2$ and a singlet $\phi_H$ charged under $U(1)_H$. The SM Higgs doublet $H_1$ as well as all the SM fermions and three…

High Energy Physics - Phenomenology · Physics 2023-11-27 Sumit Ghosh , Pyungwon Ko

A singlet fermion which interacts only with a new singlet scalar provides a viable and minimal scenario that can explain the dark matter. The singlet fermion is the dark matter particle whereas the new scalar mixes with the Higgs boson…

High Energy Physics - Phenomenology · Physics 2013-10-30 Sonja Esch , Michael Klasen , Carlos E. Yaguna

In the conventional left-right gauge model, if the Higgs scalar sector consists only of an $SU(2)_L$ doublet and an $SU(2)_R$ doublet, fermion masses are zero at tree level. There have been many studies on how they would become massive.…

High Energy Physics - Phenomenology · Physics 2021-05-19 Ernest Ma

We propose Dirac type active neutrino with rank two mass matrix and a Majorana fermion dark matter candidate with an alternative local $U(1)_{B-L}$ extension of neutrinophilic two Higgs doublet model. Our dark matter candidate can be…

High Energy Physics - Phenomenology · Physics 2018-04-04 Takaaki Nomura , Hiroshi Okada

A dynamical symmetry breaking model of electroweak interactions is investigated based on strongly interacting fermions. Vector-like fermions of different representations of the weak SU(2) form a symmetry breaking condensate and generate the…

High Energy Physics - Phenomenology · Physics 2015-03-18 G. Cynolter , E. Lendvai

We present a study of singlet-doublet vector-like leptonic dark matter (DM) in the framework of two Higgs doublet model (2HDM), where the dark sector is comprised of one doublet and one singlet vectorlike fermions (VLFs). The DM, that…

High Energy Physics - Phenomenology · Physics 2020-04-01 Basabendu Barman , Amit Dutta Banik , Avik Paul

We construct a model based on an extra gauge symmetry, SU(2)_X x U(1)_{B-L}, which can provide gauge bosons to serve as weakly-interacting massive particle dark matter. The stability of the dark matter is naturally guaranteed by a discrete…

High Energy Physics - Phenomenology · Physics 2014-03-07 Cheng-Wei Chiang , Takaaki Nomura , Jusak Tandean

We present a classically scale-invariant model where the dark matter, neutrino and electroweak mass scales are dynamically generated from dimensionless couplings. The Standard Model gauge sector is extended by a dark $SU(2)_X$ gauge…

High Energy Physics - Phenomenology · Physics 2016-03-29 Alexandros Karam , Kyriakos Tamvakis

Thermal dark matter scenarios based on light (sub-GeV) fermions typically require the presence of an extra dark sector containing both a massive dark photon along with a dark Higgs boson. The latter generates both the dark photon mass and…

High Energy Physics - Phenomenology · Physics 2018-12-26 Luc Darmé , Soumya Rao , Leszek Roszkowski

We study an extension of the Standard Model featuring a hidden sector that consists of a new scalar charged under a new SU$(N)_D$ gauge group, singlet under all Standard Model gauge interactions, and coupled with the Standard Model only via…

High Energy Physics - Phenomenology · Physics 2016-01-27 Stefano Di Chiara , Kimmo Tuominen

We investigate a two-component dark matter scenario in the type-I two-Higgs-doublet model. The dark sector contains a real scalar $s$ and a Dirac fermion $\chi$, whose stability is ensured by a $Z_4$ symmetry together with kinematic…

High Energy Physics - Phenomenology · Physics 2026-03-20 Patricio Escalona , Jacinto P. Neto , M. J. Neves , Camila Ramos , David Suarez

Several constructions motivate the existence of a dark $U(1)_D$ gauge boson which interacts with the Standard Model only through its kinetic mixing or loop induced processes. We describe two typical examples with specific signatures in…

High Energy Physics - Phenomenology · Physics 2015-03-17 Yann Mambrini

We consider the Standard Model extended by a hidden sector U(1)_X symmetry that is spontaneously broken at the TeV scale by the vacuum expectation value of an additional scalar field. We study "dark string" solutions in this model and their…

High Energy Physics - Phenomenology · Physics 2014-03-26 Jeffrey M. Hyde , Andrew J. Long , Tanmay Vachaspati

We propose a $U(1)_{B-L}$ gauge extension to the SM, in which the dark sector is stabilized through a matter parity symmetry preserved after spontaneous symmetry breaking. The fermion spectrum includes three neutral right-handed fields with…

High Energy Physics - Phenomenology · Physics 2025-08-14 Yadir Garnica , América Morales , Carlos A. Vaquera-Araujo

We study the Dark Matter (DM) discovery prospect and its spin discrimination in the theoretical framework of gauge invariant and renormalizable Higgs portal DM models at the ILC with $\sqrt{s} = 500$ GeV. In such models, the DM pair is…

High Energy Physics - Phenomenology · Physics 2017-10-25 Teruki Kamon , P. Ko , Jinmian Li

We study the renormalizable singlet-doublet fermionic extension of the Standard Model. In this model, the new vector-like fermions couple to the gauge bosons and to the Higgs via new Yukawa couplings, that allow for nontrivial mixing in the…

High Energy Physics - Phenomenology · Physics 2015-12-21 G. Cynolter , J. Kovacs , E. Lendvai

We consider a class of fermionic dark matter candidates that are charged under both the SU(2)$_L$ and U(1)$_Y$ gauge interactions. In this case a certain amount of dark matter-Higgs couplings, which can split the dark matter into a pair of…

High Energy Physics - Phenomenology · Physics 2015-04-08 Natsumi Nagata , Satoshi Shirai

We propose a seesaw model with a hidden gauge symmetry $SU(2)_H \times U(1)_X$ where two types of standard model singlet fermions in realizing a seesaw mechanism are organized into $SU(2)_H$ doublet. Then we formulate scalar and gauge…

High Energy Physics - Phenomenology · Physics 2019-12-11 Takaaki Nomura , Hiroshi Okada

We propose a minimal extension of the standard model with U(1)_{B-L} \times Z_{2} symmetry. In this model by assuming that the neutrinos are Dirac (i.e. $B-L$ is an exact symmetry), we found a simultaneous solution for non zero neutrino…

High Energy Physics - Phenomenology · Physics 2018-10-17 Nimmala Narendra , Nirakar Sahoo , Narendra Sahu

We discuss a new SU(3)_C X SU(3)_L X U(1)_X X U(1)_N (3-3-1-1) gauge model that overhauls the theoretical and phenomenological aspects of the known 3-3-1 models. Additionally, we sift the outcome of the 3-3-1-1 model from precise…

High Energy Physics - Phenomenology · Physics 2014-10-28 P. V. Dong , D. T. Huong , Farinaldo S. Queiroz , N. T. Thuy