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Related papers: A comment on the lepton mixing matrix

200 papers

Experimental results indicate a possible relation between the lepton and quark mixing matrices of the form U_PMNS \approx V_CKM^\dagger U_X, where U_X is a matrix with special structure related to the mechanism of neutrino mass generation.…

High Energy Physics - Phenomenology · Physics 2015-10-21 P. O. Ludl , A. Yu. Smirnov

We argue that flavour mixing, both in the quark and lepton sector, follows the minimal mixing pattern, according to which the whole of this mixing is basically determined by the physical mass generation for the first family of fermions. So,…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. L. Chkareuli , C. D. Froggatt , H. B. Nielsen

We construct a model of quark-lepton unification at the TeV scale based on an $SU(4)$ gauge symmetry, while still having acceptable neutrino masses and enough suppression in flavor changing neutral currents. An approximate $U(2)$ flavor…

High Energy Physics - Phenomenology · Physics 2018-05-16 Admir Greljo , Ben A. Stefanek

Recent results from lattice QCD calculations relevant to particle physics phenomenology are reviewed. They include the calculations of strong coupling constant, quark masses, kaon matrix elements, and D and B meson matrix elements. Special…

High Energy Physics - Phenomenology · Physics 2009-11-10 Shoji Hashimoto

Based on a new approach (the so-called Yukawaon model) to the mass spectra and mixings, a neutrino mass matrix which is described in terms of the up-quark masses and CKM matrix parameters is proposed. The mass matrix successfully leads to a…

High Energy Physics - Phenomenology · Physics 2009-08-20 Yoshio Koide

The quark-lepton complementarity (QLC) relations indicate a deep structure that interrelates quarks and leptons. We propose new scenarios, in a seesaw framework with discrete $A_4$ flavor symmetry, which can accommodate the QLC relations…

High Energy Physics - Phenomenology · Physics 2011-05-12 Y. H. Ahn , Hai-Yang Cheng , Sechul Oh

The non-Abelian discrete symmetry D(7) of the heptagon is successfully applied to both quark and lepton mass matrices, including CP violation.

High Energy Physics - Phenomenology · Physics 2013-02-27 Subhaditya Bhattacharya , Ernest Ma , Alexander Natale , Daniel Wegman

A parameter free, model independent analysis of quark mass matrices is carried out. We find a representation in terms of a diagonal mass matrix for the down (up) quarks and a suitable matrix for the up (down) quarks, such that the mass…

High Energy Physics - Phenomenology · Physics 2011-02-01 D. Falcone , O. Pisanti , L. Rosa

Generally the diagonalization of the mass matrix of the charged leptons is a part of the neutrino UPMNS matrix. However, usually this contribution is ignored by assuming a diagonal mass matrix for charged leptons. In this letter we test…

High Energy Physics - Phenomenology · Physics 2015-06-03 Giovanna Cottin , Marco Aurelio Diaz , Benjamin Koch

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

Using unitarity, unlike the approaches available in the literature, we have constructed 9 independent representations of CKM matrix starting with each of the 9 elements of the matrix. The relationship of these independently constructed…

High Energy Physics - Phenomenology · Physics 2024-06-25 Gurjit Kaur , Aakriti Bagai , Gulsheen Ahuja , Manmohan Gupta

We describe a solution to a long standing puzzle about the difference in textures of quark CKM and lepton PMNS mixing matrices by deriving their common representation. We show how the difference in texture of the two matrices arises from…

High Energy Physics - Phenomenology · Physics 2012-09-11 Alexander N. Jourjine

The status of lattice calculations of heavy quark phenomenology is reviewed. Particular emphasis is placed on the understanding and control of the calculational uncertainties. The ensuing implications for constraining the CKM matrix…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sinead Ryan

Texture matrices are a way of mitigating the redundancy inherent in the description of flavor physics via Yukawa couplings by eliminating some entries in order to identify relevant parameters. A four-zero texture scheme has been used in the…

High Energy Physics - Phenomenology · Physics 2021-05-05 S. Gómez-Ávila , L. López-Lozano , Pedro Miranda-Romagnoli , R. Noriega-Papaqui , Pedro Lagos-Eulogio

A simple breaking of the subnuclear democracy of the quarks leads to a mixing between the second and the third family, in agrement with observation. Introducing the mixing between the first and the second family, one finds an interesting…

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

Despite the flexibility and popularity of mixture models, their associated parameter spaces are often difficult to represent due to fundamental identification problems. This paper looks at a novel way of representing such a space for…

Methodology · Statistics 2015-10-16 Vahed Maroufy , Paul Marriott

An interesting mass relation between down type quarks and charged leptons has been recently predicted within a supersymmetric SU(3)_c \times SU(2)_L \times U(1)_Y model based on the A4 flavor symmetry. Here we propose a simple extension…

High Energy Physics - Phenomenology · Physics 2013-08-02 S. Morisi , M. Nebot , Ketan M. Patel , E. Peinado , J. W. F. Valle

The pattern of quark and lepton mass matrices is unexplained in the standard model of particle interactions. I propose the novel idea of a progressive gauge U(1) symmetry where it is a reflection of the regressive electroweak symmetry…

High Energy Physics - Phenomenology · Physics 2016-08-10 Ernest Ma

We use hyperbolic functions to parametrize lepton mixing matrix using only one input parameter $\phi$. This matrix has three mixing angles as outputs therefore giving two predictions. In particular it predicts $U_{e3}=0$ besides predicting…

High Energy Physics - Phenomenology · Physics 2010-11-11 Biswajoy Brahmachari

In the simplest model of horizontal U(1) symmetry with one singlet added to the supersymmetric standard model, we systematically reconstruct quark mass matrices from the low-energy data to prove that there are only two mass matrices found…

High Energy Physics - Phenomenology · Physics 2015-06-25 E. J. Chun , A. Lukas