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Related papers: Mass relations among quarks and/or leptons

200 papers

Against the conventional picture that the mass matrix forms in the quark sectors will take somewhat different structures from those in the lepton sectors, a possibility that all the mass matrices of quarks and leptons have the same form as…

High Energy Physics - Phenomenology · Physics 2017-08-23 Yoshio Koide , Hiroyuki Nishiura , Koichi Matsuda , Tatsuru Kikuchi , Takeshi Fukuyama

The mass formulae for the baryon octet and decuplet are calculated. These formulae are function of constituent quark masses and spin spin interaction terms for the quarks inside the baryons. The coefficients in the mass formulae is…

High Energy Physics - Phenomenology · Physics 2018-01-08 Amanpreet Kaur , Alka Upadhyay

The calculation of the quartic mass terms at order \alpha_s^3 to the hadronic R ratio is described. It is based on the operator product expansion for the quark current correlator, combined with an application of the renormalization group…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. G. Chetyrkin , R. Harlander , J. H. Kuehn

The relation between the on-shell and $\bar{\rm MS}$ mass can be expressed through scalar and vector part of the quark propagator. In principle these two-point functions have to be evaluated on-shell which is a non-trivial task at…

High Energy Physics - Phenomenology · Physics 2008-11-26 K. G. Chetyrkin , M. Steinhauser

A comparative analysis of a number of phenomenological relationships between constants of the extended Standard Model of electromagnetic, strong and weak interactions of fundamental particles (hereinafter referred to as the extended…

High Energy Physics - Phenomenology · Physics 2025-08-12 V. V. Khruschov , S. V. Fomichev

We obtain estimates of several hadron mass ratios, for Wilson quarks in the valence (quenched) approximation, extrapolated to physical quark mass, infinite volume and zero lattice spacing.

High Energy Physics - Lattice · Physics 2009-10-22 F. Butler , H. Chen , A. Vaccarino , J. Sexton , D. Weingarten

In the model every quark or lepton is identified with a quartet of four "more elementary" particles. One particle in a quartet is a massive spin-0 boson and other three particles are massless spin-1/2 fermions.

High Energy Physics - Phenomenology · Physics 2007-05-23 N. G. Marchuk

Recently, we proposed a unified mass matrix model for quarks and leptons, in which, mass ratios and mixings of the quarks and neutrinos are described by using only the observed charged lepton mass values as family-number-dependent…

High Energy Physics - Phenomenology · Physics 2016-08-03 Yoshio Koide , Hiroyuki Nishiura

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

For some time the measured value of tau-lepton mass continues to approach closer and closer a particular figure 1776.80 MeV predicted by an intrinsically composite model of three generations of leptons and quarks, introduced almost two…

High Energy Physics - Phenomenology · Physics 2010-09-27 Wojciech Krolikowski

The relativistic three-quark equations are found in the framework of the dispersion relation technique. The approximate solutions of these equations using the method based on the extraction of leading singularities of the amplitude are…

High Energy Physics - Phenomenology · Physics 2007-05-23 D. V. Ivanov

Masses of the ground-state teraquarks composed from heavy $c$ and $b$ quarks and antiquarks are calculated in the diquark-antidiquark picture in the framework of the relativistic quark model based on the quasipotential approach. The…

High Energy Physics - Phenomenology · Physics 2021-01-12 R. N. Faustov , V. O. Galkin , E. M. Savchenko

We assume that all quark and lepton mass matrices have upper triangular form. Using all available experimental data on quark and lepton masses and mixing angles we make a fit in which we determine mass matrices elements. There are too many…

High Energy Physics - Phenomenology · Physics 2008-12-19 Stanislaw Tatur , Jan Bartelski

A model is presented that fits the quark and lepton masses and mixings wherein five dimensionless parameters and a phase account for fifteen dimensionless observables. Among these are the Wolfenstein parameters $\rho$ and $\eta$, the…

High Energy Physics - Phenomenology · Physics 2011-05-12 Carl H. Albright , S. M. Barr

The starting point in this note is the charged-lepton mass formula successfully predicting the figure m_\tau = 1776.80 MeV for \tau-lepton mass versus its recent experimental value m_\tau = 1776.82 \pm 0.16 MeV. There, two experimental…

General Physics · Physics 2010-11-05 Wojciech Krolikowski

Double parton distributions can be computed from the perturbative splitting of one parton into two if the distance between the two observed partons is small. We develop schemes to take into account quark mass effects in this computation,…

High Energy Physics - Phenomenology · Physics 2023-09-25 Markus Diehl , Riccardo Nagar , Peter Plößl

We propose the lepton mixing matrix at high energy scale to be connected to quark mixing matrix by the similar transformation. The similarity between CKM and PMNS significantly narrows down the ranges in physical parameters. The condition…

High Energy Physics - Phenomenology · Physics 2010-08-23 Seungsu Hwang , Kim Siyeon

The paper collects the various pieces of information concerning the relative size of m_u, m_d and m_s. A coherent picture results, which constrains the mass ratios to a rather narrow range: m_u/m_d = 0.553 \pm 0.043, m_s/m_d = 18.9 \pm 0.8.

High Energy Physics - Phenomenology · Physics 2008-11-26 H. Leutwyler

There are eight quarks in each family and there are three families of quarks i.e. c, b, t. Also, we propose similar structure for leptons. The nature of strong force is named as `third order electroweak'.

High Energy Physics - Phenomenology · Physics 2007-05-23 Amjad Hussain Shah Gilani

Masses and mixings of quarks and leptons differ wildly from one another. Thus it is all the more challenging to search for some hidden attribute that they may share.

High Energy Physics - Phenomenology · Physics 2011-06-17 Sheldon Lee Glashow