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Related papers: Anomalous Flavor U(1)_X for Everything

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We argue that in certain models with family symmetries the implementation of the alignment mechanism for the supression of the flavor changing neutral currents requires mass matrices with holomorphic zeros in the down quark sector.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Nikolaos Irges

Heavy singlet neutrinos admit Majorana masses which are not possible for the Standard Model particles. This suggest new possibilities for generating the masses and mixing angles of light neutrinos. We present a model of neutrino physics…

High Energy Physics - Phenomenology · Physics 2008-11-26 Micheal S. Berger , Samuel Santana

We argue that simpler fermionic contents, responsible for the extension of the standard model with gauged lepton and baryon charges, can be constructed by assuming existence of so-called leptoquarks (j,k) with exotic electric charges…

High Energy Physics - Phenomenology · Physics 2017-05-25 P. V. Dong , H. N. Long

The supersymmetric extension of the standard model suffers from a problem of baryon-number violation. Discrete (and global) symmetries introduced to protect the proton are unstable under gravitational effects. We add a gauged $U(1)_X$ to…

High Energy Physics - Phenomenology · Physics 2009-10-28 A. H. Chamseddine , Herbi Dreiner

It is shown that it is possible to create successful models of flavor for both quarks and leptons using the discrete non-abelian group $T^{\prime}$ by itself. Two simple realizations are presented that can be used as the starting point for…

High Energy Physics - Phenomenology · Physics 2008-11-26 Alfredo Aranda

We first time show that a common solution to dark matter and the flavor problem of the standard model can be obtained in the framework of the $\mathcal{Z}_{\rm N} \times \mathcal{Z}_{\rm M}$ flavor symmetry where the flavonic Goldstone…

High Energy Physics - Phenomenology · Physics 2023-12-29 Gauhar Abbas , Rathin Adhikari , Eung Jin Chun

Without assuming any specific flavor symmetry and/or any specific mass matrix forms, it is demonstrated that if a flavor symmetry (a discrete symmetry, a U(1) symmetry, and so on) exists, we cannot obtain the CKM quark mixing matrix $V$ and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Yoshio Koide

Flavour physics is a priceless window on physics beyond the Standard Model. In particular, flavour violation in the lepton sector looks very promising, as high precision measurements are prospected in future experiments investigating on…

High Energy Physics - Phenomenology · Physics 2013-11-19 R. Alonso , M. B. Gavela , D. Hernandez , L. Merlo , S. Rigolin

We consider an $U(1)_{L_\mu -L_\tau}$ extended left-right symmetric gauge theory where the neutrino masses are generated through inverse seesaw mechanism. In this model the muon $(g-2)$ anomaly is accounted for by the mediation of…

High Energy Physics - Phenomenology · Physics 2022-11-04 Chayan Majumdar , Supriya Senapati , S. Uma Sankar , Urjit A. Yajnik

We present a supersymmetric model of flavor. A single U(1) gauge group is responsible for both generating the flavor spectrum and communicating supersymmetry breaking to the visible sector. The problem of Flavor Changing Neutral Currents is…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Elazzar Kaplan , Francois Lepeintre , Antonio Masiero , Ann E. Nelson , Antonio Riotto

Phenomenological implications of neutrino oscillations implied by recent experimental data on pattern of neutrino mass matrix are disscussed. It is shown that it is possible to have a neutrino mass matrix which shows approximate flavor…

High Energy Physics - Phenomenology · Physics 2009-11-10 Riazuddin

Theories of flavor operate at various scales. Recently it has been pointed out that in the context of modular flavor symmetries certain combinations of observables are highly constrained, or even uniquely fixed, by modular invariance and…

High Energy Physics - Phenomenology · Physics 2026-03-25 Mu-Chun Chen , Shaheed Perez , Michael Ratz

We propose a new $\mathrm{SU}(3)_C \otimes \mathrm{SU}(2)_{L}\otimes \mathrm{U}(1)_{Y}\otimes \mathrm{U}(1)_{X}$ gauge model which is non universal respect to the three fermion families of the Standard Model. We introduce additional one…

High Energy Physics - Phenomenology · Physics 2018-08-22 R. Martinez , S. F. Mantilla

We explore a gauged $U(1)_{B-L}$ extension of standard model with inclusion of three right-handed neutrinos of exotic $B-L$ charges to cancel the gauge anomaly. Non-trivial transformation of new particles under $B-L$ symmetry forbids the…

High Energy Physics - Phenomenology · Physics 2022-07-13 Subhasmita Mishra , Nimmala Narendra , Prafulla Kumar Panda , Nirakar Sahoo

A phenomenological approach for the universal mass matrix model with a broken flavor 2 <-> 3 symmetry is explored by introducing the 2 <-> 3 antisymmetric parts of mass matrices for quarks and charged leptons . We present explicit texture…

High Energy Physics - Phenomenology · Physics 2009-11-11 Koichi Matsuda , Hiroyuki Nishiura

The neutrino sector offers one of the most sensitive probes of new physics beyond the Standard Model of Particle Physics. The mechanism of neutrino mass generation is still unknown. The observed suppression of neutrino masses hints at a…

High Energy Physics - Phenomenology · Physics 2022-04-20 Yahya Almumin , Mu-Chun Chen , Murong Cheng , Victor Knapp-Perez , Yulun Li , Adreja Mondol , Saul Ramos-Sanchez , Michael Ratz , Shreya Shukla

We propose that all light fermionic degrees of freedom, including the Standard Model (SM) fermions and all possible light beyond-the-standard-model fields, are chiral with respect to some spontaneously broken abelian gauge symmetry.…

High Energy Physics - Phenomenology · Physics 2015-07-06 André de Gouvea , Daniel Hernandez

New mechanism of generating flavor mass spectrum is proposed by using an O'Raifeartaigh-type supersymmetry breaking model. A desired bilinear form of fermion mass spectrum is naturally realized through F-components of gauge-singlet (nonet…

High Energy Physics - Phenomenology · Physics 2009-01-06 Naoyuki Haba , Yoshio Koide

We add an energy-independent Hamiltonian to the standard flavour oscillation one. This kind of physics might appear in theories where neutrinos couple differently to a plausible non-zero torsion of the gravitational field or more…

High Energy Physics - Phenomenology · Physics 2009-08-21 M. Bustamante , A. M. Gago , C. Pena-Garay

In string compactifications, frequently there appears the anomalous U(1) gauge symmetry which belonged to E8$\times$E8 of the heterotic string. This anomalous U(1) gauge boson obtains mass at the compactification scale, just below…

High Energy Physics - Phenomenology · Physics 2017-12-13 Jihn E. Kim , Bumseok Kyae , Soonkeon Nam