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If the scale dependence of a Yukawa matrix is assumed to be determined entirely by the dominant 33-element, then the renormalization group equations can be expressed in terms of two separate equations: a differential equation for the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Bipin R. Desai , Alexander R. Vaucher

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

It is known that chiral fermions naturally appear at certain intersections of branes at angles. Motivated by this fact, we propose a string scenario in which different standard model gauge interactions propagate on different (intersecting)…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. Aldazabal , S. Franco , L. E. Ibanez , R. Rabadan , A. M. Uranga

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

Typically in unified theories the neutrino mixing angles, like the Cabibbo-Kobayashi-Maskawa (CKM) angles of the quarks, are related to the small mass ratios between fermions of different generations and are therefore quite small. A new…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , S. M. Barr

We construct a model based on the electroweak gauge group $\rm SU(2)_L \times SU(2)_R \times U(1)_{B-L}$ augmented by an $S_3$ symmetry. We assign nontrivial $S_3$ transformation properties to the quarks and consequently we need two scalar…

High Energy Physics - Phenomenology · Physics 2018-12-12 Dipankar Das , Palash B. Pal

The structure of the Cabibbo-Kobayashi-Maskawa (CKM) matrix is analyzed from the standpoint of a composite model. A model is constructed with three families of quarks, by taking tensor products of sufficient numbers of spin-1/2…

High Energy Physics - Phenomenology · Physics 2009-10-22 Jonathan L. Rosner , Mihir P. Worah

We explore a mechanism for generating the Yukawa hierarchies by displacing the left- and right-handed components of the Standard Model fermions in a higher-dimensional space. We find a unique configuration of displacements which fits all…

High Energy Physics - Phenomenology · Physics 2009-10-31 Eugene A. Mirabelli , Martin Schmaltz

In this letter we analyse, in the context of the general 2-Higgs Doublet Model, the structure of the Yukawa matrices, $\widetilde{ \bf Y}_{ _{1,2} }^{q}$, by assuming a four-zero texture ansatz for their definition. In this framework, we…

High Energy Physics - Phenomenology · Physics 2015-02-11 O. Félix-Beltrán , F. González-Canales , J. Hernández-Sánchez , S. Moretti , R. Noriega-Papaqui , A. Rosado

In a supersymmetric model with hierarchical squark masses we analyze a pattern of flavour symmetry breaking centered on the special role of the top Yukawa coupling and, by extension, of the full Yukawa couplings for the up-type quarks. For…

High Energy Physics - Phenomenology · Physics 2011-02-15 Riccardo Barbieri , Enrico Bertuzzo , Marco Farina , Paolo Lodone , Dmitry Zhuridov

We present a new mechanism, which does not require any flavor symmetry, to explain the small Yukawa couplings and CKM mixing angles. The Yukawa matrices are assumed to be random at short distances and the hierarchical structure is generated…

High Energy Physics - Phenomenology · Physics 2009-10-31 Ann E. Nelson , Matthew J. Strassler

We discuss the hierarchy of Yukawa couplings in a supersymmetric three family Standard-like string Model. The model is constructed by compactifying Type IIA string theory on a Z_2 x Z_2 orientifold in which the Standard Model matter fields…

High Energy Physics - Theory · Physics 2009-09-17 Mirjam Cvetic , Paul Langacker , Gary Shiu

We construct a multiscalar and non-renormalizable model where the $\mathbf{S}_{3}$ flavor symmetry drives mainly the Yukawa couplings. In the quark sector, the Nearest Neighbor Interaction (NNI) textures are behind the CKM mixing matrix so…

High Energy Physics - Phenomenology · Physics 2020-11-25 J. D. García-Aguilar , Juan Carlos Gómez-Izquierdo

We briefly describe a three-family intersecting D6-brane model in Type IIA theory on the T^6/(Z_2 x Z_2) orientifold with a realistic phenomenology. In this model, the gauge symmetry can be broken down to the Standard Model (SM) gauge…

High Energy Physics - Theory · Physics 2008-11-26 Ching-Ming Chen , Tianjun Li , V. E. Mayes , Dimitri V. Nanopoulos

In the context of the supersymmetric unification model in which the massless sector contains extra particles beyond those in the minimal supersymmetric standard model, we obtain mixings between quarks (leptons) and the extra particles which…

High Energy Physics - Phenomenology · Physics 2009-10-31 Takeo Matsuoka

We assume the universal Yukawa coupling (democratic mass matrix) with small violations for quarks, charged leptons and neutrinos masses. We could reproduce the mass hierarchy for quark masses and V_{CKM} matrix elements precisely. We adopt…

High Energy Physics - Phenomenology · Physics 2009-10-31 T. Teshima , T. Asai

All quark mass matrices with texture zeroes obtained through weak basis transformations are confronted with the experimental data. The reconstruction of the quark mass matrices M_u and M_d at the electroweak scale is performed in a weak…

High Energy Physics - Phenomenology · Physics 2013-05-29 D. Emmanuel-Costa , C. Simoes

We introduce a new parametrization of the MNS lepton mixing matrix which separates the hierarchical Grand Unified relations among quarks and leptons. We argue that one large angle stems from the charged leptons, the other from the seesaw…

High Energy Physics - Phenomenology · Physics 2010-04-05 Aseshkrishna Datta , Fu-Sin Ling , Pierre Ramond

We consider Yukawa couplings generated by a configuration of intersecting seven-branes in F-theory. In configurations with a single interaction point and no fluxes turned on, the Yukawa matrices have rank one. This is no longer true when…

High Energy Physics - Theory · Physics 2010-07-15 Sergio Cecotti , Miranda C. N. Cheng , Jonathan J. Heckman , Cumrun Vafa

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