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Semi-annihilation is a generic feature of dark matter theories with symmetries larger than Z_2. We explore a model based on a Z_4-symmetric dark sector comprised of a scalar singlet and a "wino"-like fermion SU(2)_L triplet. This is the…

High Energy Physics - Phenomenology · Physics 2015-10-09 Andrew P. Spray , Yi Cai

We present a detailed study of a combined singlet-doublet fermion and triplet scalar model for dark matter. These models have only been studied separately in the past. Together, they form a simple extension of the Standard Model that can…

High Energy Physics - Phenomenology · Physics 2019-05-09 Juri Fiaschi , Michael Klasen , Simon May

We propose a vector dark matter model with an exotic dark SU(2) gauge group. Two Higgs triplets are introduced to spontaneously break the symmetry. All of the dark gauge bosons become massive, and the lightest one is a viable vector DM…

High Energy Physics - Phenomenology · Physics 2021-07-28 Zexi Hu , Chengfeng Cai , Yi-Lei Tang , Zhao-Huan Yu , Hong-Hao Zhang

A dark sector resembling the standard model, where the abundance of matter is explained by baryon and lepton asymmetries, and stable constituents bind to form atoms, is a theoretically appealing possibility. We show that a minimal model…

High Energy Physics - Phenomenology · Physics 2015-12-23 Jeremie Choquette , James M. Cline

Assuming three light neutrinos and the see-saw mechanism we present a semiquantitative model of fermion masses based on (SUSY) SU(5) and abelian horizontal charges. A good description of the observed pattern of quark and lepton masses is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Guido Altarelli , Ferruccio Feruglio

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 studied a left-right symmetric model that can accommodate the neutrino dark energy (\nd) proposal. Type III seesaw mechanism is implemented to give masses to the neutrinos. After explaining the model, we study the consistency of the…

High Energy Physics - Phenomenology · Physics 2010-04-21 Jitesh R. Bhatt , Pei-Hong Gu , Utpal Sarkar , Santosh K. Singh

The seesaw type II mechanism is considered within the framework of a left-right chiral model with a gauge group $SU(2)_L\times SU(2)_R\times U(1)$, the lepton sector of which includes three generations of heavy Majorana neutrinos. The…

High Energy Physics - Phenomenology · Physics 2025-06-05 M. Dubinin , E. Fedotova , D. Kazarkin

Supersymmetric radiative neutrino mass models have often two dark matter candidates. One is the usual lightest neutralino with odd R parity and the other is a new neutral particle whose stability is guaranteed by a discrete symmetry that…

High Energy Physics - Phenomenology · Physics 2011-07-07 Hiroki Fukuoka , Daijiro Suematsu , Takashi Toma

An anomaly-free U(1) gauge extension of the standard model (SM) is presented. Only one Higgs doublet with a nonzero vacuum expectation is required as in the SM. New fermions and scalars as well as all SM particles transform nontrivially…

High Energy Physics - Phenomenology · Physics 2016-02-23 Rathin Adhikari , Debasish Borah , Ernest Ma

We discuss degenerate vector dark matter and dark photon that are induced from hidden $SU(2)_H$ gauge sector where it is spontaneously broken by vacuum expectation value of $SU(2)_H$ doublet. Kinetic mixing between $SU(2)_H$ and $U(1)_Y$…

High Energy Physics - Phenomenology · Physics 2024-05-30 Takaaki Nomura , Xinran Xu

Adding a second scalar doublet (eta^+,eta^0) and three neutral singlet fermions N_{1,2,3} to the Standard Model of particle interactions with a new Z_2 symmetry, it has been shown that eta^0_R or eta^0_I is a good dark-matter candidate and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernest Ma

We study a multi-component dark matter model where interactions with the Standard Model are primarily via the Higgs boson. The model contains vector-like fermions charged under $SU(2)_W \times U(1)_Y$ and under the dark gauge group,…

High Energy Physics - Phenomenology · Physics 2017-01-25 Anthony DiFranzo , Gopolang Mohlabeng

A minimal extension of the left-right symmetric model for neutrino masses that includes a vector-like singlet fermion dark matter (DM) is presented with the DM connected to the visible sector via a gauged U(1) portal. We discuss the…

High Energy Physics - Phenomenology · Physics 2018-12-17 M. J. Neves , J. A. Helaÿel-Neto , Rabindra N. Mohapatra , Nobuchika Okada

Within the framework of the Minimal Supersymmetric Standard Model (MSSM), we explore a decoupling of the parameters into separate sectors that determine consistency with collider data, the abundance of dark matter, and potential signatures…

High Energy Physics - Phenomenology · Physics 2016-07-27 Pearl Sandick

We establish a hybrid seesaw mechanism to explain small neutrino masses and predict cold dark matter candidate in the context of the B-L gauge symmetry extension of the Standard Model. In this model a new scalar doublet and two new fermion…

High Energy Physics - Phenomenology · Physics 2015-03-13 Tong Li , Wei Chao

We analyze a simple extension of the Standard Model (SM) with a dark sector composed of a scalar and a fermion, both singlets under the SM gauge group but charged under a dark sector symmetry group. Sterile neutrinos, which are singlets…

High Energy Physics - Phenomenology · Physics 2017-07-13 Miguel Escudero , Nuria Rius , Verónica Sanz

High energy accelerators may probe into dark matter and the seesaw neutrino mass scales if they are not much heavier than ~O(TeV). In the absence of supersymmetry, we extend a class of SO(10) models to predict well known cold dark matter…

High Energy Physics - Phenomenology · Physics 2011-09-27 Mina K. Parida

It is shown that in extensions of the standard model of quarks and leptons where additive lepton number $L$ is broken by two units, so that $Z_2$ lepton parity, i.e. $(-1)^L$ which is either even or odd, remains exactly conserved, there is…

High Energy Physics - Phenomenology · Physics 2015-07-08 Ernest Ma

In an endeavor to explain the light neutrino masses and dark matter (DM) simultaneously, we study a gauged $U(1)_{\rm B-L}$ extension of the standard model (SM). The neutrino masses are generated through a variant of type-II seesaw…

High Energy Physics - Phenomenology · Physics 2022-07-20 Purusottam Ghosh , Satyabrata Mahapatra , Nimmala Narendra , Narendra Sahu