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Related papers: New Origin of a Bilinear Mass Matrix Form

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Stimulated by a recent work by Sumino, on the basis of a model in which effective Yukawa coupling constants are described by vacuum expectation values of a scalar $\Phi$ with $3\times 3$ components, a possible form of the scalar potential…

High Energy Physics - Phenomenology · Physics 2013-11-26 Yoshio Koide

In the so-called ``yukawaon" model, the (effective) Yukawa coupling constants $Y_f^{eff}$ are given by vacuum expectation values (VEVs) of scalars $Y_f$ (yukawaons) with $3\times 3$ components. In the present model, all of the VEV matrices…

High Energy Physics - Phenomenology · Physics 2015-06-10 Yoshio Koide , Hiroyuki Nishiura

According to an idea that effective Yukawa coupling constants Y_f^{eff} are given vacuum expectation values < Y_f> of fields ("Yukawaons") Y_f as Y_f^{eff}=y_f < Y_f>/\Lambda, a possible superpotential form in the charged lepton sector…

High Energy Physics - Phenomenology · Physics 2010-01-15 Yoshio Koide

Recent work on a lepton mass matrix model based on an SU(3) flavor symmetry which is broken into S_4 is reviewed. The flavor structures of the masses and mixing are caused by VEVs of SU(2)_L-singlet scalars \phi which are nonets ({\bf…

High Energy Physics - Phenomenology · Physics 2007-07-09 Yoshio Koide

In the so-called yukawaon model, where effective Yukawa coupling constants Y_f^{eff} (f=e,\nu,u,d) are given by vacuum expectation values of gauge singlet scalars (yukawaons) Y_f with 3\times 3 flavor components, it is tried to give a…

High Energy Physics - Phenomenology · Physics 2010-01-14 Yoshio Koide

We present a model of fermion masses based on a minimal, non-Abelian discrete symmetry that reproduces the Yukawa matrices usually associated with U(2) theories of flavor. Mass and mixing angle relations that follow from the simple form of…

High Energy Physics - Phenomenology · Physics 2014-11-17 Alfredo Aranda , Christopher D. Carone , Richard F. Lebed

We present a renormalizable fermion mass model based on the symmetry $Q_4$ that accommodates all fermion masses and mixing angles in both the quark and lepton sectors. It requires the presence of only four SU(2) doublet scalar fields…

High Energy Physics - Phenomenology · Physics 2011-08-12 Alfredo Aranda , Cesar Bonilla , Raymundo Ramos , Alma D. Rojas

The Fermion flavor structure is investigated by bilinear decomposition of the mass matrix after EW symmetry breaking, and the roles of factorized matrices in flavor mixing and mass generation are explored. It is shown that flavor mixing can…

High Energy Physics - Phenomenology · Physics 2023-09-12 Guojun Xu , Jingjun Zhang , Chenzi Liao , Ying Zhang

Stimulated by Ma's idea which explains the tribimaximal neutrino mixing by assuming an A_4 flavor symmetry, a lepton mass matrix model is investigated. A Frogatt-Nielsen type model is assumed, and the flavor structures of the masses and…

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

We consider the generation of neutrino masses via a singly-charged scalar singlet. Under general assumptions we identify two distinct structures for the neutrino mass matrix. This yields a constraint for the antisymmetric Yukawa coupling of…

High Energy Physics - Phenomenology · Physics 2021-06-07 Tobias Felkl , Juan Herrero-Garcia , Michael A. Schmidt

Building an organized Yukawa structure of quarks and leptons is an essential mission to understand fermion mass hierarchy and flavor mixing in particle physics. Inspired by the similarity of CKM and PMNS mixings, a common mass pattern for…

High Energy Physics - Phenomenology · Physics 2023-11-16 Ying Zhang

Based on a new approach to quark and lepton masses, where the mass spectra originate in vacuum expectation values of O(3)-flavor 1+5 (gauge singlet) scalars, a neutrino mass matrix of a new type is speculated. The mass matrix is described…

High Energy Physics - Phenomenology · Physics 2009-11-13 Yoshio Koide

Why the charged lepton mass formula m_e +m_\mu +m_\tau = {2/3} (\sqrt{m_e}+\sqrt{m_\mu} +\sqrt{m_\tau})^2 is mysterious is reviewed, and guiding principles to solve the mystery are presented. According to the principles, an example of such…

High Energy Physics - Phenomenology · Physics 2007-05-23 Yoshio Koide

We present the general form of the unitary matrices keeping invariant the Majorana neutrino mass matrix of specific texture suitable for explaining oscillation data. In the case of the Tri-bimaximal pattern with two degenerate masses we…

High Energy Physics - Phenomenology · Physics 2011-02-01 E. I. Lashin , S. Nasri , E. Malkawi , N. Chamoun

According to an idea that the quark and lepton mass spectra originate in a VEV structure of a U(3)-flavor nonet scalar \Phi, the mass spectra of the down-quarks and charged leptons are investigated. The U(3) flavor symmetry is spontaneously…

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

In the Standard Model, Yukawa couplings parametrize the fermion masses and mixing angles with the exception of neutrino masses. The hierarchies and apparent regularities among the quark and lepton masses are, however, otherwise a mystery.…

High Energy Physics - Phenomenology · Physics 2022-11-07 Sudip Jana , Sophie Klett , Manfred Lindner

We discuss the predictive power of supersymmetric models with flavor symmetries, focusing on the lepton sector of the standard model. In particular, we comment on schemes in which, after certain `flavons' acquire their vacuum expectation…

High Energy Physics - Phenomenology · Physics 2013-02-27 Mu-Chun Chen , Maximilian Fallbacher , Michael Ratz , Christian Staudt

Based on an assumption that an S_4 flavor symmetry is embedded into SU(3), a lepton mass matrix model is investigated. A Frogatt-Nielsen type model is assumed, and the flavor structures of the masses and mixing are caused by VEVs of…

High Energy Physics - Phenomenology · Physics 2009-01-06 Yoshio Koide

Gauging a specific difference of lepton numbers such as $L_{\mu}-L_{\tau}$ is a popular model-building option, which gives rise to economical explanations for the muon anomalous magnetic moment. However, this choice of gauge group seems…

High Energy Physics - Phenomenology · Physics 2022-03-23 Gonzalo Alonso-Álvarez , James M. Cline

We discuss conditions under which bi-large mixing in the lepton sector is achieved assuming that all Yukawa matrices and the right-handed neutrino mass matrix have the same singular form in the leading order. Due to obvious quark lepton…

High Energy Physics - Phenomenology · Physics 2007-05-23 Radovan Dermisek
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