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Related papers: Family Gauge Symmetry and Koide's Mass Formula

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It was conjectured some time ago that an effective description of the Coulomb-confinement transition in compact U(1) lattice gauge field theory could be described by scalar QED obtained by soft breaking of the N=2 Seiberg-Witten model down…

High Energy Physics - Theory · Physics 2009-11-10 D. Espriu , L. Tagliacozzo

It is well established that the $SU(P)_L$ gauge symmetry for $P\geq 3$ can address the question of fermion generation number due to the anomaly cancellation, but it neither commutes nor closes algebraically with electric and…

High Energy Physics - Phenomenology · Physics 2019-09-11 Duong Van Loi , Phung Van Dong , Le Xuan Thuy

In the family grand unification models (fGUTs), we propose that gauge U(1)'s beyond the minimal GUT gauge group are family gauge symmetries. For the symmetry $L_\mu-L_\tau$, i.e. $Q_{2}-Q_{3}$ in our case, to be useful for the LHC anomaly,…

High Energy Physics - Phenomenology · Physics 2020-07-29 Paul H. Frampton , Sin Kyu Kang , Jihn E. Kim , Soonkeon Nam

Granting that the $SU_c(3) \times SU_L(2) \times U(1) \times SU_f(3)$ Standard Model is valid (or, partially valid), for the real world, we propose the $\mu^+ e^-$ collider in the $10^2\, GeV$ range as the family collider. This family…

High Energy Physics - Phenomenology · Physics 2014-09-24 W-Y. Pauchy Hwang

Lepton family number violation processes arise in the $SU(6)_L \otimes U(1)_Y$ model due to the presence of an extra neutral gauge boson, Z$'$, with family changing couplings, and due to the fact that this model demands the existence of…

High Energy Physics - Phenomenology · Physics 2009-10-31 U. Cotti , R. Gaitan , A. Hernandez , W. Ponce , A. Zepeda

In the framework of a mass formula proposed previously (transforming in a specific way three free parameters into three masses), a simple empirical sum rule for three charged-lepton masses is found, predicting m_\tau = 1776.9926 MeV, when…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wojciech Krolikowski

An effective theory is proposed, combining the standard gauge group $SU(3)_{C}\otimes SU(2)_{L}\otimes U(1)_{Y}$ with a horizontal discrete symmetry. By assigning appropriate charges under this discrete symmetry to the various fermion…

High Energy Physics - Phenomenology · Physics 2009-10-22 D. S. Shaw , R. R. Volkas

We present a common explanation of the fermion mass hierarchy and the large lepton mixing angles in the context of a grand unified flavor and gauge theory (GUTF). Our starting point is a SU(3)xU(1) flavor symmetry and a SO(10) GUT, a basic…

High Energy Physics - Phenomenology · Physics 2008-11-26 F. Bazzocchi , S. Morisi , M. Picariello , E. Torrente-Lujan

Unification ideas suggest an integral treatment of fermion and boson spin and gauge-group degrees of freedom. Hence, a generalized quantum field equation, based on Dirac's, is proposed and investigated which contains gauge and flavor…

High Energy Physics - Theory · Physics 2007-05-23 J. Besprosvany

The spin-charge-family theory predicts the existence of the fourth family to the observed three. The $4 \times 4$ mass matrices --- determined by the nonzero vacuum expectation values of the two triplet scalars, the gauge fields of the two…

High Energy Physics - Phenomenology · Physics 2019-02-08 A. Hernandez-Galeana , N. S. Mankoc Borstnik

We investigate symmetry breaking patterns from replicated gauge groups which generate anomaly-free and family-dependent U(1) symmetries. We discuss the extent to which these symmetries can explain the observed hierarchies of fermion masses…

High Energy Physics - Phenomenology · Physics 2009-11-10 Fu-Sin Ling , Pierre Ramond

If supersymmetry (SUSY) is not for stabilizing the electroweak energy scale, what is it used for in particle physics? We propose that it is for flavor problems. A cyclic family symmetry is introduced. Under the family symmetry, only the…

High Energy Physics - Phenomenology · Physics 2009-11-11 Chun Liu

The fermionic sector of the Standard Model of Elementary Particles emerges as the low energy limit of a single fermionic field freely propagating in a higher dimensional background. The local geometrical framework is obtained by enforcing…

High Energy Physics - Theory · Physics 2007-05-23 P. Maraner

We explore a framework for the computation of quark mass ratios and CKM mixing angles based on an SU(3) family gauge symmetry. The four ratios md/mb, ms/mb, mu/mt, and mc/mt can be fit at one-loop in the family gauge interaction. The same…

High Energy Physics - Phenomenology · Physics 2009-11-11 Thomas Appelquist , Yang Bai , Maurizio Piai

We present a model of quark and lepton masses and mixings based on A4 family symmetry, a discrete subgroup of an SO(3) flavour symmetry, together with Pati-Salam unification. It accommodates tri-bimaximal neutrino mixing via constrained…

High Energy Physics - Phenomenology · Physics 2010-04-06 Stephen F. King , Michal Malinsky

The family symmetry $SU(3)\otimes U(1)$ is proposed to solve flavor problems about fermion masses and flavor mixings. It's breaking is implemented by some flavon fields at the high-energy scale. In addition a discrete group $Z_{2}$ is…

High Energy Physics - Phenomenology · Physics 2015-05-30 Wei-Min Yang , Qi Wang , Jin-Jin Zhong

We propose a model in which $A_4$ Family Symmetry arises dynamically from a six dimensional orbifold SU(5) Supersymmetric Grand Unified Theory. The SU(5) is broken to the Standard Model gauge group by a particular orbifold compactification…

High Energy Physics - Phenomenology · Physics 2010-05-07 T. J. Burrows , S. F. King

It is shown that the efficient mass formula we found for charged leptons in 1992 can be considered as an excellent approximate solution to the mysterious charged-lepton mass equation proposed by Koide in 1981.

High Energy Physics - Phenomenology · Physics 2007-05-23 Wojciech Krolikowski

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

We present a simple $U(1)_{B_3-3L_\mu}$ gauge Standard Model extension that can easily account for the anomalies in $R(K)$ and $R(K^*)$ reported by LHCb. The model is economical in its setup and particle content. Among the Standard Model…

High Energy Physics - Phenomenology · Physics 2018-11-07 Cesar Bonilla , Tanmoy Modak , Rahul Srivastava , Jose W. F. Valle
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