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Related papers: 3-3-1-1 model for dark matter

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We show that the typical 3-3-1 models are only self-consistent if they contain interactions explicitly violating the lepton number. The 3-3-1 model with right-handed neutrinos can by itself work as an economical 3-3-1 model as a natural…

High Energy Physics - Phenomenology · Physics 2013-11-21 P. V. Dong , T. Phong Nguyen , D. V. Soa

Dark matter stability can result from a residual matter-parity symmetry, following naturally from the spontaneous breaking of the gauge symmetry. Here we explore this idea in the context of the $\mathrm{SU(3)_c \otimes SU(3)_L \otimes…

High Energy Physics - Phenomenology · Physics 2020-02-24 Julio Leite , Oleg Popov , Rahul Srivastava , José W. F. Valle

We present a non-supersymmetric scenario in which the R-parity symmetry $R_P = (-1)^{3(B-L)+2s}$ arises as a result of spontaneous gauge symmetry breaking, leading to a viable Dirac fermion WIMP dark matter candidate. Direct detection in…

High Energy Physics - Phenomenology · Physics 2017-10-11 Alexandre Alves , Giorgio Arcadi , P. V. Dong , Laura Duarte , Farinaldo S. Queiroz , José W. F. Valle

We argue that neutrino mass and dark matter can arise from an approximate $B-L$ symmetry. This idea can be realized in a minimal setup of the flipped 3-3-1 model, which discriminates lepton families while keeping universal quark families…

High Energy Physics - Phenomenology · Physics 2020-05-22 Duong Van Loi , Phung Van Dong , Dang Van Soa

We point out that a class of non-supersymmetric models based on the gauge group $SU(3)_C \times SU(2)_L\times SU(2)_R\times U(1)_{Y_L}\times U(1)_{Y_R}$ possesses an automatic, exact $Z_{2 }$ symmetry under which the fermions in the…

High Energy Physics - Phenomenology · Physics 2016-11-16 P. S. Bhupal Dev , Rabindra N. Mohapatra , Yongchao Zhang

In this work we show that the supersymmetric economical SU(3)_C X SU(3)_L X U(1)_X (3-3-1) gauge model has a realistic candidate for self-interacting dark matter. In the model under consideration, the right-handed sneutrino is in bottom of…

High Energy Physics - Phenomenology · Physics 2011-09-15 H. N. Long

We propose the simplest TeV-scale scotogenic extension of the original 3-3-1 theory, where dark matter stability is linked to the Dirac nature of neutrinos, which results from an unbroken $B-L$ gauge symmetry. The new gauge bosons get…

High Energy Physics - Phenomenology · Physics 2020-07-29 Julio Leite , América Morales , José W. F. Valle , Carlos A. Vaquera-Araujo

We consider a scenario where a supersymmetric model has multiple dark matter particles. Adding a U(1)' gauge symmetry is a well-motivated extension of the Minimal Supersymmetric Standard Model (MSSM). It can cure the problems of the MSSM…

High Energy Physics - Phenomenology · Physics 2008-11-26 Taeil Hur , Hye-Sung Lee , Salah Nasri

We propose a new extension of the Standard Model that incorporates a gauged \( U(1)_{\rm B-L} \) symmetry and the type-III seesaw mechanism to explain neutrino mass generation and provide a viable dark matter (DM) candidate. Unlike the…

High Energy Physics - Phenomenology · Physics 2026-01-27 Satyabrata Mahapatra , Partha Kumar Paul , Narendra Sahu , Prashant Shukla

We investigate an extension of the left-right symmetric model featuring an additional non-abelian $SU(2)$ gauge symmetry. The particle content is augmented by one generation of vector-like leptons transforming under the fundamental…

High Energy Physics - Phenomenology · Physics 2026-03-11 Yassine Bouzeraib , Mohamed Sadek Zidi , Geneviève Bélanger

Two theoretically well-motivated gauge extensions of the standard model are $SU(3)_C \times SU(3)_L \times SU(3)_R$ and $SU(3)_q \times SU(3)_L \times SU(3)_l \times SU(3)_R$, where $SU(3)_q$ is the same as $SU(3)_C$ and $SU(3)_l$ is its…

High Energy Physics - Phenomenology · Physics 2018-01-17 Corey Kownacki , Ernest Ma , Nicholas Pollard , Oleg Popov , Mohammadreza Zakeri

Dark matter is postulated to be a neutral Dirac fermion, charged under a dark $U(1)_D$ gauge symmetry. Scalar partners of the quarks and leptons are also charged under $U(1)_D$. The dark gauge boson $Z_D$ and the dark Higgs boson $h_D$…

High Energy Physics - Phenomenology · Physics 2022-07-06 Ernest Ma

We show that some models with $SU(3)_C\otimes SU(3)_L\otimes U(1)_X$ gauge symmetry can be realized at the electroweak scale and that this is a consequence of an approximate global $SU(2)_{L+R}$ symmetry. This symmetry implies a condition…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. G. Dias , J. C. Montero , V. Pleitez

WIMP dark matter and gauge coupling unification are considered in an R-parity violating MSSM with vector-like matter. Dark matter is contained in an additional vector-like SU(2)$_L$ doublet which possesses a new U(1) gauge symmetry. The…

High Energy Physics - Phenomenology · Physics 2013-05-14 Chun Liu , Jia-Shu Lu

We investigate the possibility that dark matter could be made from CP-even and CP- odd Higgs bosons in the SU(3)_C X SU(3)_L X U(1)_N (3-3-1) model with right-handed neutrinos. This self-interacting dark matters are stable without imposing…

High Energy Physics - Phenomenology · Physics 2008-11-26 Hoang Ngoc Long , Nguyen Quynh Lan

$SU(2)_L \times SU(2)_R$ gauge symmetry requires three right-handed neutrinos ($ N _i $), one of which, $N_1$, can be sufficiently stable to be dark matter. In the early universe, $ W _R $ exchange with the Standard Model thermal bath keeps…

High Energy Physics - Phenomenology · Physics 2020-09-04 Jeff A. Dror , David Dunsky , Lawrence J. Hall , Keisuke Harigaya

We propose an extension of the Standard Model gauge symmetry by the gauge group $U(1)_{T3R}$ in order to address the Yukawa coupling hierarchy between the third generation fermions and the first two generation fermions of the SM. We assume…

High Energy Physics - Phenomenology · Physics 2019-10-30 Bhaskar Dutta , Sumit Ghosh , Jason Kumar

We argue that the higher weak isospin $SU(3)_L$ manifestly unifies dark matter and normal matter in its isomultiplets for which dark matter carries a conserved dark charge while normal matter does not. The resultant gauge symmetry is given…

High Energy Physics - Phenomenology · Physics 2024-08-07 Phung Van Dong , Duong Van Loi

We propose a $B-L$ gauged extension of the Standard Model where light neutrino masses arise from type III seesaw mechanism. Unlike the minimal $B-L$ model with three right handed neutrinos having unit lepton number each, the model with…

High Energy Physics - Phenomenology · Physics 2020-03-24 Anirban Biswas , Debasish Borah , Dibyendu Nanda

In this work we study an effective version of the 3-3-1 model, in which the particle content is the same of the 2HDM. We show that the inherited structure from the $SU(3)_C \otimes SU(3)_L \otimes U(1)_X$ gauge group has a series of…

High Energy Physics - Phenomenology · Physics 2023-04-07 A. L. Cherchiglia , O. L. G. Peres