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Related papers: Hierarchical Quark Mass Matrices

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We show that solutions for the masses and mixings of the quarks and leptons based on a $U(1)\times Z_2$ horizontal symmetry are possible. The seesaw mechanism is shown to work consistently in the presence of the discrete symmetry. The…

High Energy Physics - Phenomenology · Physics 2009-10-31 Micheal S. Berger , Kim Siyeon

In a large class of supersymmetric SO(10) and left-right models, requiring that the effective theory below the scale of $SU(2)_R$ breaking be the MSSM implies partial Yukawa unification with $Y_u=Y_d$ and $Y_e=Y_{\nu^D}$. The same result…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. S. Babu , B. Dutta , R. N. Mohapatra

We construct a four-generation MSSM with rank-4 Yukawa matrices from intersecting D6 branes on a T^6/(Z_2 x Z_2) orientifold. The Yukawa matrices obtained provide an example of Flavor Democracy (FD), where the Yukawa couplings are all…

High Energy Physics - Phenomenology · Physics 2011-02-28 A. V. Belitsky , Richard F. Lebed , Van E. Mayes

The quark mixing matrix is parameterised such that its "Cabibbo substructure" is emphasised. One can choose one of the parameters to be an arbitrarily chosen angle of the unitarity triangle, for example the angle $\beta$ (also called…

High Energy Physics - Phenomenology · Physics 2009-11-11 C. Jarlskog

Fritzsch-Xing matrices are a particular class of texture 4 zero hermitian quark mass matrices, known to be successful in accommodating the quark mixing data. In the present work, it is shown that these texture 4-zero matrices with only one…

High Energy Physics - Phenomenology · Physics 2022-08-02 Nikhila Awasthi , Manoj Kumar , Monika Randhawa , Manmohan Gupta

The idea of a rank-one rotating mass matrix (R2M2) is reviewed detailing how it leads to ready explanations both for the fermion mass hierarchy and for the distinctive mixing patterns between up and down fermion states, which can be and…

High Energy Physics - Phenomenology · Physics 2015-05-27 Michael J Baker , J. Bordes , H. M. Chan , S. T. Tsou

Noting the hierarchy between three mixing angles, $\theta_{2,3}={\cal O}(\theta_1^2)$, we present an exact form of the quark mixing matrix, replacing Wolfenstein's approximate form. In addition, we suggest to rotate the unitarity triangle,…

High Energy Physics - Phenomenology · Physics 2015-05-28 Jihn E. Kim , Min-Seok Seo

We explain the imbalance of the flavor mixing angles between the quark and the lepton sectors in the context of the SU(5) GUT with the see-saw mechanism. The quark masses and the CKM matrix elements are obtained by using, respectively, the…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. Hagiwara , N. Okamura

We show that the Standard Model Yukawa matrices satisfy a set of simple yet nontrivial inequalities. The relations we derive are independent of the basis used to define the fermion fields, and, amongst other things, place strong constraints…

High Energy Physics - Phenomenology · Physics 2025-06-10 Gero von Gersdorff , Lucas Modesto

In view of the observed strong hierarchy of the quark and lepton masses and of the flavor mixing angles it is argued that the description of flavor mixing must take this into account. One particular interesting way to describe the flavor…

High Energy Physics - Phenomenology · Physics 2007-05-23 Harald Fritzsch

We study systematically the possibility for realizing realistic values of quark mass ratios $m_c/m_t$ and $m_s/m_b$ and the mixing angle $V_{cb}$ by using only renormalizable Yukawa couplings derived from heterotic orbifold models. We…

High Energy Physics - Phenomenology · Physics 2009-11-10 Pyungwon Ko , Tatsuo Kobayashi , Jae-hyeon Park

Although different parametrizations of quark mixing matrix are mathematically equivalent, the consequences of experimental analysis may be distinct. Based on the triminimal expansion of Kobayashi-Maskawa matrix around the unit matrix, we…

High Energy Physics - Phenomenology · Physics 2011-01-27 Nan Qin , Bo-Qiang Ma

The Standard Model does not constrain the form of the Yukawa matrices and thus the origin of fermion mass hierarchies and mixing pattern remains puzzling. On the other hand, there are intriguing relations between fermion masses and mixing…

High Energy Physics - Phenomenology · Physics 2023-05-02 Benedetta Belfatto , Zurab Berezhiani

To address fermion mass hierarchy and flavor mixings in the quark and lepton sectors, a minimal flavor structure without any redundant parameters beyond phenomenological observables is proposed via decomposition of the Standard Model Yukawa…

High Energy Physics - Phenomenology · Physics 2022-01-17 Ying Zhang

We propose a bottom-up approach that a structure of a high-energy physics is explored by accumulating existence proofs and/or no-go theorems in the standard model or its extension. As an illustration, we study fermion mass hierarchies based…

High Energy Physics - Phenomenology · Physics 2020-05-06 Yoshiharu Kawamura

On the basis of the Froggatt-Nielsen mechanism, we study quark flavor mixings in the $SU(6) \times SU(2)_R$ model. The characteristic structure of the CKM matrix is attributed to the hierarchical effective Yukawa couplings due to the…

High Energy Physics - Phenomenology · Physics 2016-06-22 Chuichiro Hattori , Masahisa Matsuda , Mamoru Matsunaga , Takeo Matsuoka

We present a framework to generate the quark mass hierarchies and mixing angles by extending the Standard Model with one extra Higgs doublet. The charm and strange quark masses are generated by small quantum effects, thus explaining the…

High Energy Physics - Phenomenology · Physics 2015-06-19 Alejandro Ibarra , Ana Solaguren-Beascoa

A flavor structure with minimal parameters is proposed to address the fermion mass hierarchy and flavor mixing for quarks and leptons. Yukawa interaction is reconstructed in a new basis to show a homological flat structure for up-type…

High Energy Physics - Phenomenology · Physics 2023-02-14 Ying Zhang

A nearly historical account of quark mass matrix models is given, and the structure of quark mass matrices in the Standard Model is studied. For a minimal parameter basis suggested earlier, where $M_u$ is diagonal and $M_{d11}$, $M_{d13}$,…

High Energy Physics - Phenomenology · Physics 2014-11-17 D. Falcone

We assume that all quark and lepton $3 \times 3$ mass matrices which appear in the standard model lagrangian (after spontaneous symmetry breaking) with neutrinos treated as Dirac patricles have the triangular form. Such matrices have not…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Tatur , J. Bartelski