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Clifford Unification describes all the observed fundamental fermions in terms of seven commuting elements of the $Cl_{7,7}$ Clifford algebra. The eigenvalues of each commuting element define a binary quantum number, which relates to a…

General Physics · Physics 2026-03-04 Douglas Newman

It is shown that for a higher weak isospin symmetry, $SU(P)_L$ with $P\geq 3$, the baryon minus lepton charge $B-L$ neither commutes nor closes algebraically with $SU(P)_L$ similar to the electric charge $Q$, which all lead to a…

High Energy Physics - Phenomenology · Physics 2020-12-15 Cao H. Nam , Duong Van Loi , Le Xuan Thuy , Phung Van Dong

We explore the dark matter and collider phenomenology of the minimal gauged $U(1)_B$ model, consisting of a leptophobic $Z_B$ gauge boson, and an accompanying Higgs $S_B$. By requirement of anomaly cancellation, the fermion sector naturally…

High Energy Physics - Phenomenology · Physics 2015-09-23 Sebastian Ohmer , Hiren H. Patel

We argue that neutrino mass and dark matter can arise from an approximate $B-L$ symmetry. This idea can be realized in a minimal setup of the flipped 3-3-1 model, which discriminates lepton families while keeping universal quark families…

High Energy Physics - Phenomenology · Physics 2020-05-22 Duong Van Loi , Phung Van Dong , Dang Van Soa

We investigate scenarios in which dark matter is stabilized by an abelian Z_N discrete gauge symmetry. Models are surveyed according to symmetries and matter content. Multi-component dark matter arises when N is not prime and Z_N contains…

High Energy Physics - Phenomenology · Physics 2011-02-18 Brian Batell

We reexamine sterile neutrino dark matter in gauged $U(1)_{B-L}$ model. Improvements have been made by tracing and careful evaluation of the evolution of the number densities of sterile neutrinos $N$ and extra neutral gauge bosons $Z'$. As…

High Energy Physics - Phenomenology · Physics 2022-11-30 Shintaro Eijima , Osamu Seto , Takashi Shimomura

Superheavy dark matter can satisfy the observed dark matter abundance if the stability condition is fulfilled. Here, we propose a new Abelian gauge symmetry ${\rm U(1)}_H$ for the stability of superheavy dark matter as the electromagnetic…

High Energy Physics - Phenomenology · Physics 2015-06-23 Jong-Chul Park , Seong Chan Park

We analyze the dynamics of an $SU_L(2)\otimes U_R(1)$ chiral gauge theory on a lattice with a large multifermion coupling $1\ll g_2 < \infty$. It is shown that no spontaneous symmetry breaking occurs; the ``spectator'' fermion $\psi_R(x)$…

High Energy Physics - Lattice · Physics 2008-02-03 She-Sheng Xue

On the basis of an observation due to Kiskis, Narayanan and Neuberger, we show that there is a remnant of chiral anomalies in the reduced model when a Dirac operator which obeys the Ginsparg-Wilson relation is employed for the fermion…

High Energy Physics - Lattice · Physics 2009-11-07 Yoshio Kikukawa , Hiroshi Suzuki

In this work, we explore an extension of the Standard Model designed to elucidate the fermion mass hierarchy, account for the dark matter relic abundance, and explain the observed matter-antimatter asymmetry in the universe. Beyond the…

High Energy Physics - Phenomenology · Physics 2024-09-04 Carolina Arbeláez , A. E. Cárcamo Hernández , Claudio Dib , Patricio Escalona Contreras , Vishnudath K. N. , Alfonso Zerwekh

The radiative seesaw model with gauged $\mathrm{U(1)}_{B-L}\times\mathbb{Z}_2$ extension is a well-motivated scenario which gives consistent predictions of active neutrino masses and the abundance of dark matter. Majorana masses of…

High Energy Physics - Phenomenology · Physics 2024-10-31 Shinya Kanemura , Yushi Mura , Guohao Ying

We investigate a simple theory where Baryon number (B) and Lepton number (L) are local gauge symmetries. In this theory B and L are on the same footing and the anomalies are cancelled by adding a single new fermionic generation. There is an…

High Energy Physics - Phenomenology · Physics 2014-11-20 Pavel Fileviez Perez , Mark B. Wise

Since the electric charge in the standard model is theoretically not quantized, we may have a variant of it, called dark charge. Similar to the electric charge, the dark charge neither commutes nor closes algebraically with $SU(2)_L$. The…

High Energy Physics - Phenomenology · Physics 2022-08-18 Duong Van Loi , Nguyen Manh Duc , Phung Van Dong

We propose the family universal $U(1)_X$ models with three right-handed neutrinos by choosing the $U(1)_X$ gauge symmetry as a linear combination of $U(1)_Y\times U(1)_{\chi}$ of $SO(10)$. To be consistent with the quantum gravity effects,…

High Energy Physics - Phenomenology · Physics 2022-10-13 Tianjun Li , Qianfei Xiang , Xiangwei Yin , Han Zhou

We study a dark matter model with local B-3L_i symmetry that is known as anomaly free and requires a single right-handed neutrino. Here we have two dark matter candidates; that is, fermionic or bosonic one. We focus on analyzing each of the…

High Energy Physics - Phenomenology · Physics 2012-12-04 Hiroshi Okada

In this letter we consider that assuming: a) that the only left-handed neutral fermions are the active neutrinos, b) that $B-L$ is a gauge symmetry, and c) that the $L$ assignment is restricted to the integer numbers, the anomaly…

High Energy Physics - Phenomenology · Physics 2009-05-29 J. C. Montero , V. Pleitez

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

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 consider a supersymmetric model with extra $U(1)_B \times U(1)_L$ gauge symmetry that are broken spontaneously. Salient features of this model are that there are three different types of cold dark matter (CDM) candidates, and neutral…

High Energy Physics - Phenomenology · Physics 2011-06-28 Pyungwon Ko , Yuji Omura

I suggest a minimal extension of the SM with $U(1)_{B-L}\otimes Z_{2}$. It can simultaneously accommodate the tiny neutrino mass, cold dark mater and baryon asymmetry besides the SM. All of the new physics arise from the $U(1)_{B-L}$…

High Energy Physics - Phenomenology · Physics 2017-04-27 Wei-Min Yang
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