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Related papers: Reconstruction of quark mass matrices in the NNI f…

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For three generations of quarks, we show that one of quark mass matrices can be transformed into either a Fritzsch form or a Branco-Silva-Marcos form, while the other is kept in the NNI basis. In these bases, quark mass matrices are…

High Energy Physics - Phenomenology · Physics 2009-10-30 Eiichi Takasugi

It is pointed out that the phase convention of the CKM matrix V affects texture analysis of the quark mass matrices (M_u, M_d) when we try to describe (M_u, M_d) by the observable quantities (quark masses and CKM matrix parameters) only.…

High Energy Physics - Phenomenology · Physics 2009-10-30 Yoshio Koide

A physical model which describes the CKM matrix is analyzed. The elements of such a matrix are field-strength renormalization factors. Each column gives the probability amplitude for the field operators of the coupled Lagrangian to create a…

High Energy Physics - Phenomenology · Physics 2007-05-23 E. Sassaroli

Using a set of rephasing-invariant variables, it is shown that the renormalization group equations for quark mixing parameters can be written in a form that is compact, in addition to having simple properties under flavor permutation. We…

High Energy Physics - Phenomenology · Physics 2016-05-16 S. H. Chiu , T. K. Kuo

We propose a new and efficient method of reconstructing quark mass matrices from their eigenvalues and a complete set of mixing observables. By a combination of the principle of NNI (nearest neighbour interaction) bases which are known to…

High Energy Physics - Phenomenology · Physics 2009-11-07 Silke Falk , Rainer Hausling , Florian Scheck

In the Standard Model, we obtain a non-Fritzsch like configuration with five texture zeros for the quark mass matrices. This matrix generates the quark masses, the inner angles of the CKM unitary triangle, and the CP-violating phase in the…

High Energy Physics - Phenomenology · Physics 2018-11-14 Yithsbey Giraldo , Eduardo Rojas

In the light of several recent analyses pointing towards texture 4-zero Fritzsch-like quark mass matrices as the only viable structures for quark mass matrices, this work adopts a model independent approach to reconstruct an alternate and…

High Energy Physics - Phenomenology · Physics 2017-08-31 Rohit Verma

We review two recently proposed on-shell schemes for the renormalization of the Cabibbo-Kobayashi-Maskawa (CKM) quark mixing matrix in the Standard Model. One first constructs gauge-independent mass counterterm matrices for the up- and…

High Energy Physics - Phenomenology · Physics 2010-01-15 B. A. Kniehl , A. Sirlin

We perform an analysis of general quark mass matrices in the general nearest neighbor interaction form. Excellent agreement with experiment is realized with this general texture, which is neither hermitian nor real-symmetric. We then…

High Energy Physics - Phenomenology · Physics 2009-10-31 David Dooling , Kyungsik Kang

We examine the unitarity triangle of the KM matrix by using the general quark mass matrices on the NNI basis. The Fritzsch anz\"atz is modified by introducing four additional parameters. The KM matrix elements are expressed in terms of…

High Energy Physics - Phenomenology · Physics 2010-11-23 Toshiaki Ito , Morimitsu Tanimoto

We obtain explicitly the renormalization group equations for the quark mass matrices in terms of a set of rephasing invariant parameters. For a range of assumed high energy values for the mass ratios and mixing parameters, they are found to…

High Energy Physics - Phenomenology · Physics 2010-04-21 Shao-Hsuan Chiu , T. K. Kuo , Tae-Hun Lee , Chi Xiong

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 analyze properties of general quark mass matrices. The up and down part quark mass matrices are written in terms of six dimensionless parameters and six quark masses. It is shown that two of the former six dimensionless parameters can be…

High Energy Physics - Phenomenology · Physics 2011-04-12 K. Harayama , N. Okamura

We briefly review existing proposals for the renormalization of the Cabibbo-Kobayashi-Maskawa (CKM) matrix and study the numerical effects of several of them on the W-boson hadronic partial decay widths. We then use these results to…

High Energy Physics - Phenomenology · Physics 2014-11-18 A. A. Almasy , B. A. Kniehl , A. Sirlin

The renormalization factor relating the bare to the renormalization group invariant quark masses is accurately calculated in quenched lattice QCD using a recursive finite-size technique. The result is presented in the form of a product of a…

High Energy Physics - Lattice · Physics 2009-10-31 Stefano Capitani , Martin Lüscher , Rainer Sommer , Hartmut Wittig

We investigate how the Fritzsch ansatz for the quark mass matrices can be modified in the least possible way to accommodate the observed large top quark mass and the measured values of the CKM elements. As one of the solutions, we find that…

High Energy Physics - Phenomenology · Physics 2009-10-28 B. Dutta , S. Nandi

Every nonsingular fermion mass matrix, by an appropriate unitary transformation of right-chiral fields, is equivalent to a triangular matrix. Using the freedom in choosing bases of right-chiral fields in the minimal standard model,…

High Energy Physics - Phenomenology · Physics 2009-10-30 R. Haeussling , F. Scheck

A modified Fritzsch ansatz for the quark mass matrices is proposed to account for the hierarchical structure of the CKM matrix. To allow for the observed CP asymmetry, restrictions have to be imposed on the relative phase degree of freedom…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. K. Sze

We reconstruct the Standard Model (SM) quark masses and the Cabibbo-Kobayashi-Maskawa (CKM) matrix from a five-dimensional model, with the fifth dimension compactified on an S^1/Z_2 orbifold. Fermions are localized only at the orbifold…

High Energy Physics - Phenomenology · Physics 2014-11-17 A. Soddu , N-K. Tran

We obtain constraints on possible structures of mass matrices in the quark sector by using as experimental restrictions the determined values of the quark masses at the $M_Z$ energy scale, the magnitudes of the quark mixing matrix elements…

High Energy Physics - Phenomenology · Physics 2008-11-26 S. Chaturvedi , V. Gupta , G. Sanchez-Colon
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