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Related papers: Kinetic mixing effect in noncommutative $B-L$ gaug…

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We examine spontaneous symmetry breaking of a renormalisable U(1) x U(1) gauge theory coupled to fermions when kinetic mixing is present. We do not assume that the kinetic mixing parameter is small. A rotation plus scaling is used to remove…

High Energy Physics - Phenomenology · Physics 2014-09-09 Biswajoy Brahmachari , Amitava Raychaudhuri

We show that the mixing effect of the neutral gauge bosons in the 3-3-1-1 model comes from two sources. The first one is due to the 3-3-1-1 gauge symmetry breaking as usual, whereas the second one results from the kinetic mixing between the…

High Energy Physics - Phenomenology · Physics 2016-06-03 P. V. Dong , D. T. Si

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 present two models where the familiar leptonic symmetry $L_e-L_\mu-L_\tau$ is a gauge symmetry. We show how anomaly cancellation constrains the allowed theories, with one of them requiring a fourth sequential chiral standard model…

High Energy Physics - Phenomenology · Physics 2023-07-19 Satyabrata Mahapatra , Rabindra N. Mohapatra , Narendra Sahu

We consider a U(1) gauge theory, minimally coupled to a massless Dirac field, where a higher-derivative term is added to the pure gauge sector, as in the Lee-Wick models. We find that this term can trigger chiral symmetry breaking at low…

High Energy Physics - Phenomenology · Physics 2008-11-26 Emidio Gabrielli

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

The gauged $U(1)_{L_\mu-L_\tau}$ extension of the Standard Model is a very simple framework that can alleviate the tension in muon anomalous magnetic dipole moment, reinforced by the recent Fermilab measurement. We explore experimental…

High Energy Physics - Phenomenology · Physics 2022-02-02 Timothy Hapitas , Douglas Tuckler , Yue Zhang

It is well-known that the charge of fermion is 0 or $\pm1$ in the U(1) gauge theory on noncommutative spacetime. Since the deviation from the standard model in particle physics has not yet observed, and so there may be no room to…

High Energy Physics - Theory · Physics 2007-05-23 Yoshitaka Okumura

We discuss dynamical breaking of non-abelian gauge groups in three dimensional (lattice) gauge systems via the formation of fermion condensates. A physically relevant example, motivated by condensed-matter physics, is that of a fermionic…

High Energy Physics - Lattice · Physics 2016-09-01 K. Farakos , N. E. Mavromatos

Extensions of the standard model with a $U(1)$ gauge symmetry contain gauge invariant kinetic mixing, $\sin\chi$, and gauge non-invariant mass mixing, $\delta M^2$, between the hypercharge and the new gauge boson $Z'$. These represent a…

High Energy Physics - Phenomenology · Physics 2020-03-05 Anjan S. Joshipura , Namit Mahajan , Ketan M. Patel

We consider a gauge symmetry extension of the standard model given by $SU(3)_C\otimes SU(2)_L\otimes U(1)_X\otimes U(1)_N\otimes Z_2$ with minimal particle content, where $X$ and $N$ are family dependent but determining the hypercharge as…

High Energy Physics - Phenomenology · Physics 2023-11-15 Duong Van Loi , Cao H. Nam , Phung Van Dong

The most general Lagrangian for a model with two U(1) gauge symmetries contains a renormalizable operator which mixes their gauge kinetic terms. Such kinetic mixing can be generated at arbitrarily high scales but will not be suppressed by…

High Energy Physics - Phenomenology · Physics 2009-07-09 Keith R. Dienes , Christopher Kolda , John March-Russell

The structure of the quark and lepton masses and mixing angles provides one of the few windows we have on the underlying physics generating the \sm. In an attempt to identify the underlying symmetry group we look for the simplest gauge…

High Energy Physics - Phenomenology · Physics 2011-07-19 Luis E. Ibanez , G. G. Ross

The cosmological baryon asymmetry can be explained as remnant of heavy Majorana neutrino decays in the early universe. We study this mechanism for two models of neutrino masses with a large \nu_\mu-\nu_\tau mixing angle which are based on…

High Energy Physics - Phenomenology · Physics 2009-10-31 W. Buchmuller , M. Plumacher

Assuming all three known neutrinos are Dirac fermions, $U(1)_{B-L}$ can be an exact symmetry. We show that, if the condition of charge quantization is relaxed, the anomaly-free $B-L$ charges of two out of three right-handed neutrinos can be…

High Energy Physics - Phenomenology · Physics 2026-01-22 Xiyuan Gao , Amir N. Khan

We study quark and lepton mass matrix textures in a model containing an additional $U(1)_X$ gauge symmetry with origins in string compactification. The $U(1)_X$ symmetry is broken near the string scale, and we assume that the anomalies are…

High Energy Physics - Phenomenology · Physics 2016-08-24 Merle Michael Robinson , Jacek Ziabicki

We study a model with $U(1)$ gauged lepton number symmetry in which the active neutrino masses are generated at two-loop level through the spontaneous breaking of the lepton number symmetry. To cancel gauge anomalies some exotic leptons are…

High Energy Physics - Phenomenology · Physics 2017-06-06 Takaaki Nomura , Hiroshi Okada

We analyze a model with unbroken B-L gauge symmetry where neutrino masses are generated at one loop, after spontaneous breaking of a global U(1) symmetry. These symmetries ensure dark matter stability and the Diracness of neutrinos. Within…

High Energy Physics - Phenomenology · Physics 2021-05-14 Carlos Alvarado , Cesar Bonilla , Julio Leite , José W. F. Valle

We report new results for lattice gauge theories with twelve fermion flavors in the fundamental representation and two fermion flavors in the two-index symmetric (sextet) representation of the SU(3) color gauge group. Both models are…

High Energy Physics - Lattice · Physics 2011-04-01 Zoltan Fodor , Kieran Holland , Julius Kuti , Daniel Nogradi , Chris Schroeder

We show that under a new U(1) gauge symmetry, which is non-anomalous in the presence of one ``right-handed neutrino'' per generation and consistent with the standard model Yukawa couplings, the most general fermion charges are determined in…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mu-Chun Chen , Andre de Gouvea , Bogdan A. Dobrescu
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