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Related papers: Unification for the Darkly Charged Dark Matter

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We explain the electron-positron excess reported by the DAMPE collaboration recently in a radiative Dirac seesaw model where a dark $U(1)_X$ gauge symmetry can (i) forbid the tree-level Yukawa couplings of three right-handed neutrinos to…

High Energy Physics - Phenomenology · Physics 2017-12-05 Pei-Hong Gu

We propose a scalar dark matter model featuring a hidden gauge symmetry, denoted as U(1)_X, with two complex scalars, Phi and S. In this framework, Phi spontaneously breaks the U(1)_X gauge symmetry, while S serves as a viable dark matter…

High Energy Physics - Phenomenology · Physics 2025-05-20 Yu-Hang Su , Chengfeng Cai , Yu-Pan Zeng , Hong-Hao Zhang

We analyze a recently proposed extension of the Standard Model based on the SU(4) x SU(2)_L x U(1)_X gauge group, in which baryon number is interpreted as the fourth color and dark matter emerges as a neutral partner of the ordinary quarks…

High Energy Physics - Phenomenology · Physics 2016-04-13 Bartosz Fornal , Tim M. P. Tait

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

The recent high energy electron and positron flux observed by the DAMPE experiment indicates possible excess events near 1.4 TeV. Such an excess may be evidence of dark matter annihilations or decays in a dark matter subhalo that is located…

High Energy Physics - Phenomenology · Physics 2018-08-22 Xuewen Liu , Zuowei Liu

The minimal standard model of quarks and leptons is extended with a set of vectorlike fermions to allow baryon number $B$ to become a gauged $U(1)_B$ symmetry. The $B$ assignments of the new particles are determined by renormalizable…

High Energy Physics - Phenomenology · Physics 2021-01-13 Ernest Ma

I build a SU(2)left x U(1) electroweak gauge theory of J=0 mesons, which transform like sets of fermion-antifermion composite fields. SU(2)left x U(1) is embedded in a natural way, compatible with the Glashow-Salam-Weinberg model for…

High Energy Physics - Phenomenology · Physics 2007-05-23 B. Machet

We consider the Standard Model (SM) extended by a secluded $U(1)_D$ gauge sector encompassing a Dirac fermion ($\chi$) dark matter (DM), an abelian gauge boson $Z^\prime$ and a SM-singlet complex-scalar field $\Phi$, whose radial component…

High Energy Physics - Phenomenology · Physics 2026-04-28 Avirup Ghosh , Alexei H. Sopov , Raymond R. Volkas

Dark Matter models that employ a vector portal to a dark sector are usually treated as an effective theory that incorporates kinetic mixing of the photon with a new U(1) gauge boson, with the $Z$ boson integrated out. However, a more…

High Energy Physics - Phenomenology · Physics 2024-04-16 Miguel P. Bento , Howard E. Haber , João P. Silva

Minimal dark matter is an attractive candidate for dark matter because it is stabilized without the need to impose additional symmetries. It is known that the $SU(2)_L$ quintuplet fermion can serve as a minimal dark matter candidate, with…

High Energy Physics - Phenomenology · Physics 2025-03-26 Takashi Toma

A model for electroweak unification of quarks and leptons, in a gauge group $SU_{C}(3)\times SU(4)\times U_{X}(1)$ is constructed. The model requires, three generations of quarks and leptons which are replicas (mirror) of the standard…

High Energy Physics - Phenomenology · Physics 2015-06-03 Fayyazuddin

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

We present a simplified version of the atomic dark matter scenario, in which charged dark constituents are bound into atoms analogous to hydrogen by a massless hidden sector U(1) gauge interaction. Previous studies have assumed that…

High Energy Physics - Phenomenology · Physics 2013-05-30 James M. Cline , Zuowei Liu , Wei Xue

We extend the Dirac Scotogenic model with the aim of realizing neutrino masses together with the mass of a keV-scale dark matter (DM) candidate via the same one-loop topology. Two of the Standard Model (SM) neutrinos become massive Dirac…

High Energy Physics - Phenomenology · Physics 2022-09-26 Maximilian Berbig

We argue that the gauge symmetry which includes SU(3)_L as a higher weak-isospin symmetry is manifestly given by SU(3)_C\otimes SU(3)_L\otimes U(1)_X\otimes U(1)_N, where the last two factors determine the electric charge and B-L,…

High Energy Physics - Phenomenology · Physics 2015-09-22 P. V. Dong

We analyze the direct detection signals of a toy model consisting of a Dirac dark matter particle which couples to one Standard Model fermion via a scalar mediator. For all scenarios, the dark matter particle scatters off nucleons via one…

High Energy Physics - Phenomenology · Physics 2015-06-03 Alejandro Ibarra , Sebastian Wild

We propose an inverse seesaw scenario under hidden $U(1)$ gauge symmetry, having rather natural hierarchies among neutral fermion mass scales. The hierarchies are derived from theory and experimental constraints. The theory requires…

High Energy Physics - Phenomenology · Physics 2022-08-24 Takaaki Nomura , Hiroshi Okada , Prasenjit Sanyal

We present a model of partial compositeness arising as the IR limit of a SU(4) gauge theory with only fermionic matter. This group is one of the most promising ones among a handful of possible choices allowing a symmetry breaking pattern…

High Energy Physics - Phenomenology · Physics 2015-06-19 Gabriele Ferretti

We show that a scalar and a fermion charged under a global U(1) symmetry can not only explain the existence and abundance of dark matter (DM) and dark radiation (DR), but also imbue DM with improved scattering properties at galactic scales,…

High Energy Physics - Phenomenology · Physics 2014-10-21 Xiaoyong Chu , Basudeb Dasgupta

Asymmetric dark matter is a well-motivated approach to explain the apparent coincidence between the relic densities of visible and dark matter, $\Omega_D \simeq 5.4\Omega_b$. A complete explanation requires two components, a relation…

High Energy Physics - Phenomenology · Physics 2026-03-04 Peter Cox , Rafael E. Pérez , Raymond R. Volkas