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Related papers: Unifying the electroweak and B-L interactions

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A cosmological model is introduced in which dark matter plays a dominant role throughout the history of the universe, and is the only matter present for temperatures $T \gtrsim T_{15} \sim 10^9$ GeV. The gauge group is $SU(3) \times…

High Energy Physics - Phenomenology · Physics 2015-05-08 Paul H. Frampton , Pham Q. Hung

After some general remarks about SU_L(4) electroweak unification, the model is extended to SU_L(4)xU_X(1) to accomodate fractionally charged quarks. The unification scale is expected to be in TeV region. A right-handed Majorana neutrino…

High Energy Physics - Phenomenology · Physics 2008-11-26 Fayyazuddin , Riazuddin

We present a minimal left-right dark matter framework that can simultaneously explain the recently observed 3.55 keV X-ray line from several galaxy clusters and gauge coupling unification at high energy scale. Adopting a minimal dark matter…

High Energy Physics - Phenomenology · Physics 2017-12-27 Debasish Borah , Arnab Dasgupta , Sudhanwa Patra

We consider the possibility that dark matter is stabilised by a discrete $Z_2$ symmetry which arises from a subgroup of a $U(1)'$ gauge symmetry, spontaneously broken by integer charged scalars, and under which the chiral quarks and leptons…

High Energy Physics - Phenomenology · Physics 2022-01-05 Bowen Fu , Stephen F. King

We consider electroweak-charged dark matter in an $SO(10)$ unified theory that solves the strong $CP$ problem via Parity. Electroweak-charged dark matter has a colored $SO(10)$ partner, whose mass should be much above the dark matter mass…

High Energy Physics - Phenomenology · Physics 2024-07-03 Matthew J. Baldwin , Keisuke Harigaya

We introduce a new class of $U(1)_X$ symmetries where all Standard Model fermions are ``chiral," i.e., the left- and right-handed components have different charges under the $U(1)_X$ symmetry. Gauge anomaly cancellation is achieved by…

High Energy Physics - Phenomenology · Physics 2026-03-19 Hemant Prajapati , Rahul Srivastava

We propose a model with an $U(1)_{B-L}$ gauge symmetry, in which small neutrino masses, dark matter and the matter-antimatter asymmetry in the Universe can be simultaneously explained. In particular, the neutrino masses are generated…

High Energy Physics - Phenomenology · Physics 2018-02-19 Chao-Qiang Geng , Hiroshi Okada

We present a unified theory of inflation, neutrino mass, baryogenesis and dark matter where global lepton number symmetry and its breaking play a crucial role. The basic idea is to use a lepton number carrying complex scalar field as the…

High Energy Physics - Phenomenology · Physics 2022-03-14 Rabindra N. Mohapatra , Nobuchika Okada

The work is a brief review of the theory based on the $SU(3)_c \otimes SU(3)_L \otimes U(1)_X$ gauge group in the presence of Heavy Leptons. Recent analysis have established a set of four possible variants for the 3-3-1HL, whose content…

High Energy Physics - Phenomenology · Physics 2018-02-23 F. C. Correia

We propose a neutrino model in which neutrino masses are generated at one loop level and three right-handed fermions have non-trivial charges under $U(1)_{B-L}$ gauge symmetry in no conflict with anomaly cancellation. After the…

High Energy Physics - Phenomenology · Physics 2019-03-06 Takaaki Nomura , Hiroshi Okada

A new dynamical symmetry breaking of $SU(2)_{L}\times U(1)$ caused by the combination of the axial-vector component and the fermion mass is found in electroweak theory. We obtain (m^{2}_{W}={1/2}g^{2}m^{2}_{t}) and (m^{2}_{Z}=\rho…

High Energy Physics - Phenomenology · Physics 2016-09-06 Bing An Li

We consider models with extra U(1)' gauge symmetry that is broken spontaneously. In the models, there are cold dark matter candidates which are charged under U(1)' symmetry. Depending on the charge assignment, we can evade the strong bound…

High Energy Physics - Phenomenology · Physics 2015-06-03 Yuji Omura

We study the flavor dependent $U(1)_{B_i-L_j}$ models, where an $i$th generation of quarks and $j(\neq i)$th generation of leptons are charged. By solving the anomaly free condition for the matter sector of the SM fermions and three…

High Energy Physics - Phenomenology · Physics 2023-10-04 Nobuchika Okada , Osamu Seto

The \mu parameter of the supersymmetric standard model is replaced by \lambda S, where S is a singlet chiral superfield, introducing a Peccei--Quinn symmetry into the theory. Dynamics at the electroweak scale naturally solves both the…

High Energy Physics - Phenomenology · Physics 2014-11-18 Brian Feldstein , Lawrence J. Hall , Taizan Watari

We propose a classically scale invariant extension of the Standard Model where the electroweak symmetry breaking and the mass of the Dark Matter particle come from the common scale. We introduce $U(1)_X$ gauge symmetry and $X$-charged…

High Energy Physics - Phenomenology · Physics 2014-03-28 Branimir Radovcic , Sanjin Benic

We propose a top hypercharge model with gauge symmetry SU(3)_C x SU(2)_L x U(1)_1 x U(1)_2 where the first two families of the Standard Model (SM) fermions are charged under U(1)_1 while the third family is charged under U(1)_2. The U(1)_1…

High Energy Physics - Phenomenology · Physics 2009-01-06 Cheng-Wei Chiang , Jing Jiang , Tianjun Li , Yong-Rui Wang

Because of the problems arising from the fermion unification in the traditional Grand Unified Theory and the mass hierarchy between the 4-dimensional Planck scale and weak scale, we suggest the low energy gauge unification theory with low…

High Energy Physics - Theory · Physics 2009-11-07 Tianjun Li , Wei Liao

We propose an electroweakly interacting spin-1 dark matter (DM) model. The electroweak gauge symmetry, SU(2)$_L\times$U(1)$_Y$, is extended into SU(2)$_0\times$SU(2)$_1 \times $SU(2)$_2 \times$U(1)$_Y$. A discrete symmetry exchanging…

High Energy Physics - Phenomenology · Physics 2020-08-26 Tomohiro Abe , Motoko Fujiwara , Junji Hisano , Kohei Matsushita

We propose a minimal extension of the standard model with U(1)_{B-L} \times Z_{2} symmetry. In this model by assuming that the neutrinos are Dirac (i.e. $B-L$ is an exact symmetry), we found a simultaneous solution for non zero neutrino…

High Energy Physics - Phenomenology · Physics 2018-10-17 Nimmala Narendra , Nirakar Sahoo , Narendra Sahu

We propose an extension of the 3-3-1 model with an additional symmetry group $Z_{2}\times Z_{4} \times U(1)_{L_g}$ and an extended scalar sector. To our best knowledge this is the first example of a renormalizable 3-3-1 model, which allows…

High Energy Physics - Phenomenology · Physics 2018-10-01 A. E. Cárcamo Hernández , Sergey Kovalenko , H. N. Long , Ivan Schmidt
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