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A search for charged and neutral excited leptons is performed in 217 pb^-1 of e+e- collision data collected with the L3 detector at LEP at centre-of-mass energies from 202 GeV up to 209 GeV. The pair- and single-production mechanisms of…

High Energy Physics - Experiment · Physics 2012-08-27 L3 Collaboration

A previously developed lepton mass equation is extended to include the massive bosons and quarks of all three generations. The particles are modeled as closed, string-like, light front solitons whose key quantum numbers are their node…

High Energy Physics - Theory · Physics 2007-05-23 Roger C. Millikan , Dennis C. Richman

$\tau$ is playing an important role in the current B-physics indications from experiments of lepton flavor universality violations(LFUV). This suggests it be given increasing attention theoretically in the coming years, given also the fact…

High Energy Physics - Phenomenology · Physics 2022-11-14 Amarjit Soni

We test whether or not the tau lepton manifests the same couplings as the mu lepton by investigating the relative decay rates in purely leptonic D+ meson decays. Specifically, we place the first upper limit on the ratio R=Gamma(D+ -> tau+…

High Energy Physics - Experiment · Physics 2010-04-08 P. Rubin , CLEO Collaboration

The number of leptons may or may not be a conserved quantity. The Standard Model predicts that it is (in perturbative processes), but there is the well known possibility that new physics violates lepton number in one or two units. The first…

High Energy Physics - Phenomenology · Physics 2020-12-30 Renato M. Fonseca

It is proposed that $T$ violation in physics, as well as the masses of electron and $u, d$ quarks, arise from a pseudoscalar interaction with a new spin 0 field $\tau(x)$, odd in $P$ and $T$, but even in $C$. This interaction contains a…

High Energy Physics - Phenomenology · Physics 2009-09-28 R. Friedberg , T. D. Lee

We study quark and lepton mass matrices with the common modulus $\tau$ in the $A_4$ modular symmetry. The viable quark mass matrices are composed of modular forms of weights $2$, $4$ and $6$. It is remarked that the modulus $\tau$ is close…

High Energy Physics - Phenomenology · Physics 2020-05-05 Hiroshi Okada , Morimitsu Tanimoto

Lepton number violation and its relation to neutrino masses is investigated in several versions of the $SU(3)_c\otimes SU(3)_L\otimes U(1)_x$ model. Spontaneous and explicit violation and conservation of the lepton number are considered. In…

High Energy Physics - Phenomenology · Physics 2015-03-06 Richard H. Benavides , Luis N. Epele , Huner Fanchiotti , Carlos García Canal , William A. Ponce

It is shown that in reaction \gamma\gamma\to\ell^+\ell^-+\nu's at \sqrt{s}>200 GeV with polarized photons, large and well observable differences arise in the distribution of positive and negative charged leptons (\ell=\mu^\pm, e^\pm),…

High Energy Physics - Phenomenology · Physics 2009-02-23 D. A. Anipko , M. Cannoni , I. F. Ginzburg , K. A. Kanishev , A. V. Pak , O. Panella

Gauging a specific difference of lepton numbers such as $L_{\mu}-L_{\tau}$ is a popular model-building option, which gives rise to economical explanations for the muon anomalous magnetic moment. However, this choice of gauge group seems…

High Energy Physics - Phenomenology · Physics 2022-03-23 Gonzalo Alonso-Álvarez , James M. Cline

The 3 X 3 Majorana neutrino mass matrix is written as a sum of 3 terms, i.e. M_nu = M_A + M_B + M_C, where M_A is proportional to the identity matrix and M_B and M_C are invariant under different Z_3 transformations. This M_nu is very…

High Energy Physics - Phenomenology · Physics 2009-11-10 Ernest Ma

The recent experimental estimate for tau lepton mass comes significantly near to a theoretical value proposed by us in 1992. We recall our argumentation supporting this proposal.

High Energy Physics - Phenomenology · Physics 2014-11-18 Wojciech Krolikowski

Neutrino masses provide evidence of lepton flavour violation, but no violation in the interactions among the charged leptons has been observed yet. Many models of Physics Beyond the Standard Model (BSM) predict Charged Lepton Flavour…

High Energy Physics - Phenomenology · Physics 2023-09-15 Marco Ardu , Gianantonio Pezzullo

Some of the motivations for quark and lepton compositeness, and some problems associated with present schemes, are noted. One model is discussed in which quarks and leptons are taken as composites of spin-1/2 fermions $F$ with charges $\pm…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jonathan L. Rosner

The study of heavy-light meson masses should provide a way to determine renormalized quark masses and other properties of heavy-light mesons. In the context of lattice QCD, for example, it is possible to calculate hadronic quantities for…

High Energy Physics - Phenomenology · Physics 2018-02-14 N. Brambilla , J. Komijani , A. S. Kronfeld , A. Vairo

The three active light neutrinos are used to explain the neutrino oscillations. The inherently bi-large mixing neutrino mass matrix and the Fritzsch type, bi-small mixing charged lepton mass matrix are assumed. By requiring the maximal…

High Energy Physics - Phenomenology · Physics 2014-11-17 Chun Liu , Jeonghyeon Song

A generalization of the well-known Georgi-Jarlskog relation m_{\mu}/m_{\tau} = 3 (m_s/m_b) to neutrinos is found in the context of SO(10). This new relation is m_{\nu_\mu}/m_{\nu_\tau} = 16 (m_c/m_t), which is consistent with present data,…

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

In this paper we present the state of the art about the quarks: group SU(3), Lie algebra, the electric charge and mass. The quarks masses are generated in the same way as the lepton masses. It is constructed a term in the Lagrangian that…

General Physics · Physics 2017-06-01 Voicu Dolocan

Similarity between the weak interaction properties of quarks and leptons has led to suggestions that the origin of lepton mixing angles may be related to those of quarks. In this paper, we present a gauge model based on $SU(2)_L \times…

High Energy Physics - Phenomenology · Physics 2009-11-10 P. H. Frampton , R. N. Mohapatra

Starting from general expressions of well-chosen symmetric nuclear matter quantities derived for both zero- and finite-range effective theories, we derive the contributions to the effective mass. We first show that, independently of the…

Nuclear Theory · Physics 2018-04-18 D. Davesne , J. Navarro , J. Meyer , K. Bennaceur , A. Pastore