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Related papers: Lightest U-parity Particle (LUP) dark matter

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The Lightest Supersymmetric Particle (LSP) makes a good Dark Matter (DM) candidate, since its relic density quite naturally comes out close to the cosmologically required value. This is true even in minimal Supergravity models with…

High Energy Physics - Phenomenology · Physics 2009-09-25 M. Drees

The Minimal Supersymmetric Standard Model (MSSM) with conserved R-parity suffers from several fine-tuning problems, e.g. the mu-problem and the problem of proton decay through higher dimension operators. Both of these problems can be…

High Energy Physics - Phenomenology · Physics 2009-10-09 Hye-Sung Lee , Christoph Luhn , Konstantin T. Matchev

In the framework of an nonuniversal $U(1)'$ extension of the standard model, we propose an scalar candidate for cold dark matter which exhibits interactions with ordinary matter through Higgs and gauge bosons. Using limits from low energy…

High Energy Physics - Phenomenology · Physics 2014-11-07 R. Martinez , J. Nisperuza , F. Ochoa , J. P. Rubio

The standard model of particle physics is marvelously successful. However, it is obviously not a complete or final theory. I shall argue here that the structure of the standard model gives some quite concrete, compelling hints regarding…

High Energy Physics - Phenomenology · Physics 2009-10-28 Frank Wilczek

We consider a U(1)$_X$ gauge symmetry extension of the Standard Model (SM) with a $Z^\prime$-portal Majorana fermion dark matter that allows for a relatively light gauge boson $Z^\prime$ with mass of 10 MeV$-$ a few GeV and a much heavier…

High Energy Physics - Phenomenology · Physics 2020-10-28 Nobuchika Okada , Satomi Okada , Qaisar Shafi

A precise solution of the general relativity equations for centrally symmetric distribution of a pseudoscalar field with U(1) symmetry is presented. It is found that energy density of the field is restricted in the symmetry center and falls…

General Physics · Physics 2016-11-10 I. K. Rozgacheva , A. A. Agapov

We investigate a class of models where the supergravity model with the standard model gauge group is extended by a hidden sector $U(1)_X$ gauge group and where the lightest supersymmetric particle is the neutralino in the hidden sector. We…

High Energy Physics - Phenomenology · Physics 2019-04-03 Amin Aboubrahim , Pran Nath

We construct a little Higgs model with the most minimal extension of the standard model gauge group by an extra U(1) gauge symmetry. For specific charge assignments of scalars, an approximate U(3) global symmetry appears in the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yang Bai

We attempt to understand the baryon-dark-matter coincidence problem within the quark seesaw extension of the standard model where parity invariance is used to solve the strong CP problem. The $SU(2)_L\times SU(2)_R\times U(1)_{B-L}$ gauge…

High Energy Physics - Phenomenology · Physics 2017-09-20 Pei-Hong Gu , Rabindra N. Mohapatra

The minimal dark matter model is given a supersymmetric extension. A super SU(2)L quintuplet is introduced with its fermionic neutral component still being the dark matter, the dark matter particle mass is about 19.7 GeV. Mass splitting…

High Energy Physics - Phenomenology · Physics 2015-06-04 Xue Chang , Chun Liu , Feng-Cai Ma , Shuo Yang

Perturbative gauge coupling unification in realistic superstring models suggests the existence of additional heavy down-type quarks, beyond the minimal supersymmetric standard model. The mass scale of the heavy down-type quarks is…

High Energy Physics - Phenomenology · Physics 2009-10-28 Sanghyeon Chang , Claudio Coriano , Alon E. Faraggi

We study the prospect of heavy singlet neutrinos as a dark matter (DM) candidate within a neutrinophilic U(1) model, where the Standard Model (SM) is extended with a U(1) gauge symmetry, and neutrino mass and oscillation parameters are…

High Energy Physics - Phenomenology · Physics 2024-05-27 Waleed Abdallah , Anjan Kumar Barik , Santosh Kumar Rai , Tousik Samui

The nature of dark matter (DM) and how it might interact with the particles of the Standard Model (SM) is an ever-growing mystery. It is possible that the existence of new `dark sector' forces, yet undiscovered, are the key to solving this…

High Energy Physics - Phenomenology · Physics 2020-01-29 Thomas D. Rueter , Thomas G. Rizzo

The present matter content of our universe may be governed by a $U(1)_{B-L}$ symmetry -- the simplest gauge completion of the seesaw mechanism which produces small neutrino masses. The matter parity results as a residual gauge symmetry,…

High Energy Physics - Phenomenology · Physics 2020-12-15 Phung Van Dong , Duong Van Loi

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

A model of dark energy and dark matter was proposed earlier by one of us (PQH) which involved an unbroken gauge group $SU(2)_Z$ whose coupling $\alpha_Z \equiv g_Z^2/4 \pi\sim O(1)$ at a scale $\Lambda_Z \sim 3 \times 10^{-3} eV$ starting…

High Energy Physics - Phenomenology · Physics 2007-05-23 P. Q. Hung , Paola Mosconi

We review the role played by the '$\mu$ from $\nu$' supersymmetric standard model ($\mu \nu$SSM) in the search for supersymmetry. First, we discuss its theoretical motivation, that is the simultaneous solution of $\mu$- and $\nu$-problems…

High Energy Physics - Phenomenology · Physics 2020-12-30 Daniel E. Lopez-Fogliani , Carlos Munoz

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 Re(eta^0) or Im(eta^0) is a good dark-matter candidate…

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

We propose a simple gauged U(1)$_{B-L}$ extension of the minimal supersymmetric Standard Model (MSSM), where R-parity is conserved as usual in the MSSM. The global $B-L$ (baryon number minus lepton number) symmetry in the MSSM is gauged and…

High Energy Physics - Phenomenology · Physics 2016-03-08 Nobuchika Okada , Nathan Papapietro

We prove that the $SU(3)_C\otimes SU(2)_L \otimes SU(3)_R\otimes U(1)_X$ (3-2-3-1) gauge model always contains a matter parity $W_P=(-1)^{3(B-L)+2s}$ as conserved residual gauge symmetry, where $B-L=2(\beta T_{8R}+X)$ is a $SU(3)_R\otimes…

High Energy Physics - Phenomenology · Physics 2018-09-28 D. T. Huong , P. V. Dong , N. T. Duy , N. T. Nhuan , L. D. Thien
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