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Dark Matter (DM) being the vital ingredient in the cosmos, still remains a mystery. Standard assumption is that the collisionless cold dark matter (CCDM) particles are represented by some weakly interacting fundamental fields which can not…

Astrophysics · Physics 2009-11-11 Ariel Zhitnitsky

We consider models of accidental dark matter, namely models in which the dark matter is a composite state that is stable thanks to an accidental symmetry of the theory. The fundamental constituents are vectorlike fermions, taken to be…

High Energy Physics - Phenomenology · Physics 2024-08-12 Stefano Palmisano , Francesco Rescigno , Federica Troni

An $SU(2)_N$ extension ($N$ stands for neutral) of the Standard Model (SM) is proposed with an additional $U(1)=S^{'}$ global symmetry, which stabilizes the lightest of the vector boson ($X,\bar{X}$) as dark matter (DM) through unbroken…

High Energy Physics - Phenomenology · Physics 2018-09-26 Basabendu Barman , Subhaditya Bhattacharya , Mohammadreza Zakeri

A toy-model with $SU(2)_{\rm TC}$ dynamics confined at high scales $\Lambda_{\rm TC}\gg 100$ GeV enables to construct Dirac UV completion from the original chiral multiplets predicting a vector-like nature of their weak interactions…

High Energy Physics - Phenomenology · Physics 2016-03-18 Roman Pasechnik , Vitaly Beylin , Vladimir Kuksa , Grigory Vereshkov

We propose a new mechanism where a multi-component dark sector generates the observed dark matter abundance and baryon asymmetry and thus addresses the coincidence between the two. The thermal freeze-out of dark matter annihilating into…

High Energy Physics - Phenomenology · Physics 2022-03-08 Xiaoyong Chu , Yanou Cui , Josef Pradler , Michael Shamma

We present a simple extension of the standard model that gives rise to baryogenesis a has a dark matter candidate of O(GeV) mass. A minimal set of new fields required for baryogenesis includes two O(TeV) colored scalars and a singlet…

High Energy Physics - Phenomenology · Physics 2013-08-09 Rouzbeh Allahverdi , Bhaskar Dutta

Pure singlets are typically disfavored as dark matter candidates, since they generically have a thermal relic abundance larger than the observed value. In this paper, we propose a new dark matter mechanism called "assimilation", which takes…

High Energy Physics - Phenomenology · Physics 2012-03-08 Francesco D'Eramo , Lin Fei , Jesse Thaler

A ~5 GeV `dark baryon' with a cosmic asymmetry similar to that of baryons is a natural candidate for the dark matter. We study the possibility of generating such a state through dynamical electroweak symmetry breaking, and show that it can…

High Energy Physics - Phenomenology · Physics 2011-09-28 Mads T. Frandsen , Subir Sarkar , Kai Schmidt-Hoberg

We present a framework based on the standard type-I seesaw model that relates the baryon asymmetry of the universe to the dark matter (DM) density. The framework, which we name "Asymgenesis", relies on the presence of primordial charge…

High Energy Physics - Phenomenology · Physics 2026-03-03 Martin A. Mojahed , Sascha Weber

We propose a scenario that explains the comparable abundances of dark matter (DM) and baryons without any coincidence in the corresponding particle masses. Here, DM corresponds to heavy "dark baryons" in a hidden MSSM-like dark sector,…

High Energy Physics - Phenomenology · Physics 2022-11-21 João G. Rosa , Duarte M. C. Silva

We show how trinification models based on the gauge group $SU(3)_C \times SU(3)_L \times SU(3)_R$ realized near the TeV scale can provide naturally a variety of dark matter (DM) candidates. These models contain a discrete $T$ parity which…

High Energy Physics - Phenomenology · Physics 2022-03-02 K. S. Babu , Sudip Jana , Anil Thapa

We first suggested a scenario in which a generic, dark chiral gauge group undergoes a first order phase transition in order to generate the observed baryon asymmetry in the universe, provide a viable dark matter candidate and explain the…

High Energy Physics - Phenomenology · Physics 2012-02-15 Devin G. E. Walker

Models of inelastic (or pseudo-Dirac) dark matter commonly introduce a gauge symmetry spontaneously broken by the introduction of a dark sector version of the Higgs mechanism. We find that this ubiquitous introduction of two extra fields, a…

High Energy Physics - Phenomenology · Physics 2025-02-13 Giovani Dalla Valle Garcia

We introduce a new paradigm for dark matter (DM) interactions in which the interaction strength is asymptotically safe. In models of this type, the coupling strength is small at low energies but increases at higher energies, and…

High Energy Physics - Phenomenology · Physics 2015-09-02 Francesco Sannino , Ian M. Shoemaker

The minimal gauge group extension to the standard model (SM) by the local $U(1)_{B-L}$ (MBLSM) is well known as the minimal model to understand neutrino mass origins via the seesaw mechanism, following the gauge principle. This "small"…

High Energy Physics - Phenomenology · Physics 2018-08-22 Chengfeng Cai , Zhaofeng Kang , Hong-Hao Zhang , Yupan Zeng

We propose a two-component asymmetric FIMP (feebly interacting massive particle) dark matter (DM) model in which both DM candidates are real scalar fields. The model is an extension of the Standard Model (SM) by two scalar DM components and…

High Energy Physics - Phenomenology · Physics 2026-05-26 S. Peyman Zakeri

We present an overview of supersymmetry searches, both at collider experiments and via searches for dark matter (DM). We focus on three DM possibilities in the SUSY context: the thermally produced neutralino, a mixture of axion and axino,…

High Energy Physics - Phenomenology · Physics 2014-11-18 Howard Baer , Eun-Kyung Park , Xerxes Tata

We consider a simple class of models in which the relic density of dark matter is determined by the baryon asymmetry of the universe. In these models a $B - L$ asymmetry generated at high temperatures is transfered to the dark matter, which…

High Energy Physics - Phenomenology · Physics 2009-07-09 David E. Kaplan , Markus A. Luty , Kathryn M. Zurek

We consider scenarios where Dark Matter (DM) particles carry baryon and/or lepton numbers, which can be defined if there exist operators connecting the dark to the visible sector. As a result, the DM fields become intimately linked to the…

High Energy Physics - Phenomenology · Physics 2016-09-21 Nicolás Bernal , Chee Sheng Fong , Nayara Fonseca

Motivated by the observed ratio of dark matter to baryon mass densities, $\rho_D/\rho_B \simeq 5$, we propose a theory of dark-color unification. In this theory, the dark to visible baryon masses are fixed by the ratio of dark to visible…

High Energy Physics - Phenomenology · Physics 2022-05-18 Clara Murgui , Kathryn M. Zurek
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