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Related papers: Updated Values of Running Quark and Lepton Masses

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The predicted value of the higgs mass $m_H$ is analyzed assuming the existence of the fourth generation of leptons ($N, E$) and quarks ($U, D$). The steep and flat directions are found in the five-dimensional parameter space: $m_H$, $m_U$,…

High Energy Physics - Phenomenology · Physics 2011-01-25 V. A. Novikov , L. B. Okun , A. N. Rozanov , M. I. Vysotsky

A non-supersymmetric grand unified theory can exhibit a "radiative fermion mass hierarchy", in which the heavier quarks and leptons get mass at tree level and the lighter ones get mass from loop diagrams. Recently the first predictive model…

High Energy Physics - Phenomenology · Physics 2009-06-30 S. M. Barr , Almas Khan

The recently proposed model of neutrino mass with no new physics beyond the TeV energy scale is shown to admit a natural and realistic supersymmetric realization, when combined with another recently proposed model of quark masses in the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Ernest Ma

I report low energy results on the study of fermion masses and mixing for quarks and leptons, including neutrinos within a SU(3) flavor symmetry model, where ordinary heavy fermions, top and bottom quarks and tau lepton become massive at…

High Energy Physics - Phenomenology · Physics 2012-12-20 Albino Hernandez-Galeana

Koide's mass relation of charged leptons has been extended to quarks and neutrinos, and we prove here that this relation is independent of energy scale in a huge energy range from $1 {GeV}$ to $2\times10^{16} {GeV}$. By using the parameters…

High Energy Physics - Phenomenology · Physics 2009-11-11 Nan Li , Bo-Qiang Ma

The recent evidence for neutrino oscillations stimulate us to discuss again the problem of fermion masses and mixings in gauge theories. In the standard model, several forms for quark mass matrices are equivalent. They become ansatze within…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Falcone

The existence of extra chiral generations with all fermions heavier than M_Z is strongly disfavoured by the precision electroweak data. However the data are fitted nicely even by a few extra generations, if one allows neutral leptons to…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Maltoni , V. A. Novikov , L. B. Okun , A. N. Rozanov , M. I. Vysotsky

A new procedure is developed which enables one to start from the quark and lepton mass and mixing data at the low scale and construct mass matrices which exhibit simple SO(10) structure at the SUSY GUT scale. This approach is applied to the…

High Energy Physics - Phenomenology · Physics 2010-11-01 Carl H. Albright , Satyanarayan Nandi

Recently Babu, Ma and Valle proposed a model of quark and lepton mixing based on $A_4$ symmetry. Within this model the lepton and slepton mixings are intimately related. We perform a numerical study in order to derive the slepton masses and…

High Energy Physics - Phenomenology · Physics 2010-04-06 M. Hirsch , J. C. Romao , S. Skadhauge , J. W. F. Valle , A. Villanova del Moral

We discuss mass matrices with four texture zeros for the quarks and leptons. The three mixing angles for the quarks and leptons are functions of the fermion masses. The results agree with the experimental data. The ratio of the masses of…

High Energy Physics - Phenomenology · Physics 2015-07-29 Harald Fritzsch

Understanding the structure of the fermion mixing matrices is an important question in particle physics. The quark mixing matrix is approximately diagonal while the lepton mixing matrix has large off-diagonal elements. Attempting to…

High Energy Physics - Phenomenology · Physics 2021-02-09 Peter B. Denton

The possibility of additional quarks and leptons beyond the three generations already established is discussed. The make-up of this Report is (I) Introduction: the motivations for believing that the present litany of elementary fermions is…

High Energy Physics - Phenomenology · Physics 2009-07-09 Paul H. Frampton , P. Q. Hung , Marc Sher

We present a new measurement of the mass of the top quark using lepton + jets ttbar events collected by the DO experiment in Run I of the Fermilab Tevatron Collider. The mass is extracted through a comparison of each event with a…

High Energy Physics - Experiment · Physics 2007-05-23 V. M. Abazov , The D0 Collaboration

We calculate quark and lepton masses and quark mixing angles in the framework of a supersymmetric SU(4)$\otimes$SU(2)$_L\otimes$SU(2)$_R$ model where the gauge group is broken at 10$^{16}$ GeV. The model predicts third family top-bottom-tau…

High Energy Physics - Phenomenology · Physics 2010-11-01 B. C. Allanach , S. F. King

Observational evidences of nonzero neutrino masses and the existence of dark matter request physics beyond standard model. A model with extra scalars and leptonic vector-like fermions is introduced. By imposing a Z_2 symmetry, the neutrino…

High Energy Physics - Phenomenology · Physics 2011-04-20 Chian-Shu Chen , Chung-Hsien Chou

The {\it theory unifying spin and charges and predicting families}, proposed by N.S.M.B., predicts at the low energy regime two (in the mixing matrix elements decoupled) groups of four families. There are two kinds of contributions to mass…

High Energy Physics - Phenomenology · Physics 2011-12-20 A. Hernandez-Galeana , N. S. Mankoc Borstnik

We present an ansatz for the quark and lepton mass matrices, derivable from SO(10) type GUTs, which accommodates a heavy $(> 92 GeV)$ top quark and permits large mixings in the $\nu_\mu \leftrightarrow \nu_\tau$ sector (as suggested by the…

High Energy Physics - Phenomenology · Physics 2009-10-22 K. S. Babu , Q. Shafi

The simplest extension of the SM to account for the observed neutrino masses and mixings is the addition of at least two singlet fermions (or right-handed neutrinos). If their masses lie at or below the GeV scale, such new fermions would be…

High Energy Physics - Phenomenology · Physics 2023-09-08 Pilar Coloma , Enrique Fernandez-Martinez , Manuel Gonzalez-Lopez , Josu Hernandez-Garcia , Zarko Pavlovic

An explicit form of charged--lepton mass matrix, predicting $m_\tau = 1776.80$ MeV from the experimental values of $m_e$ and $m_\mu$ (in good agreement with the experimental figure $m_\tau = 1777.05^{+0.29}_{-0.26}$ MeV), is applied to…

High Energy Physics - Phenomenology · Physics 2007-05-23 Wojciech Krolikowski

Two vector-like families with masses of order 1 TeV, one of which is a doublet of $SU(2)_L$ and the other a doublet of $SU(2)_R$, have been predicted to exist in the context of a viable and economical SUSY composite model. One of the many…

High Energy Physics - Phenomenology · Physics 2011-05-12 K. S. Babu , Jogesh C. Pati , Hanns Stremnitzer