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Related papers: A note on Koide's lepton mass relation

200 papers

We have derived constraints on the tau neutrino mass and fourth generation mixing from an analysis of the partial widths of tau lepton decays, in particular: tau -> e nu nu_tau, tau -> mu nu nu_tau, tau -> pi nu_tau, tau -> K nu_tau. We…

High Energy Physics - Phenomenology · Physics 2008-11-26 John Swain , Lucas Taylor

It is shown that the efficient mass formula we found for charged leptons in 1992 can be considered as an excellent approximate solution to the mysterious charged-lepton mass equation proposed by Koide in 1981.

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

The perturbative quark mass corrections to the tau hadronic width are studied to O(alpha_s^3 m_q^2). Including up to dimension four corrections, we get m_s(4 GeV^2)=(143 \pm 42) MeV [m_s(1 GeV^2)=(193 \pm 59) MeV ]. Possible improvements to…

High Energy Physics - Phenomenology · Physics 2009-10-31 Joaquim Prades , Antonio Pich

Searches for new physics in events with hadronic jets, missing transverse energy, and two leptons of which at least one is a hadronically decaying tau are presented. The result is based on a data sample corresponding to an integrated…

High Energy Physics - Experiment · Physics 2019-08-13 Matthias Edelhoff

We measure the mass of the tau lepton to be 1775.1+-1.6(stat)+-1.0(syst.) MeV using tau pairs from Z0 decays. To test CPT invariance we compare the masses of the positively and negatively charged tau leptons. The relative mass difference is…

High Energy Physics - Experiment · Physics 2008-11-26 G. Abbiendi , the OPAL collaboration

The cubic symmetry S_4 contains A_4 and S_3, both of which have been used to study neutrino mass matrices. Using S_4 as the family symmetry of a complete supersymmetric theory of leptons, it is shown how the requirement of breaking S_4 at…

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

Recently, Golterman and Shamir presented an effective field theory which is supposed to describe the low-energy physics of the pion and the dilaton in an $SU(N_c)$ gauge theory with $N_f$ Dirac fermions in the fundamental representation. By…

High Energy Physics - Lattice · Physics 2017-07-27 Aya Kasai , Ken-ichi Okumura , Hiroshi Suzuki

Since the fifties, isospin relations have been used in particle physics to understand the properties of multihadrons final states. In the case of the tau lepton, they allow to relate the partial widths of the decay modes to the cross…

High Energy Physics - Phenomenology · Physics 2007-05-23 Andre Rouge

Current experimental data suggest some relations between the Kobayashi-Maskawa Matrix and the quark mass ratios, namely $|V_{us}| \sim \sqrt{m_d / m_s}$, $|V_{ub} / V_{cb}| \sim \sqrt{m_u / m_c}$ and $|V_{cb}| \sim m_s / m_b$. We consider…

High Energy Physics - Phenomenology · Physics 2009-10-31 K. Harayama

We show that linear Regge trajectories for mesons and glueballs, and the cubic mass spectrum associated with them, determine a relation between the masses of the \rho meson and the scalar glueball, M(0^{++})=3/\sqrt{2} M(\rho ), which…

High Energy Physics - Phenomenology · Physics 2010-05-27 L. Burakovsky

The analytic relation between the \bar {MS} and the pole quark masses is computed to O(\alpha_s^3) in QCD. Using this exact result, the accuracy of the large \beta_0 approximation is critically examined and the implications of the obtained…

High Energy Physics - Phenomenology · Physics 2009-10-31 Kirill Melnikov , Timo van Ritbergen

According to the Particle Data Group, the measurements of ${\cal B}(W^+ \to \tau^+ \nu_\tau)$ and ${\cal B}(W^+ \to \ell^+ \nu_\ell)$ ($\ell = e,\mu$) disagree with one another at the $2.3\sigma$ level. In this paper, we search for a…

High Energy Physics - Phenomenology · Physics 2016-05-13 Bhubanjyoti Bhattacharya , Alakabha Datta , David London

Belle II has a broad $\tau$ physics program, in particular in searches for lepton flavour and lepton number violations. Belle II profits from the relatively large $\tau$-pair production rate in the low background environment of $e^+e^-$…

High Energy Physics - Experiment · Physics 2021-11-29 Thomas Kraetzschmar

We present new constraints on the mass $m_{\nu_\tau}$ of the tau neutrino and its mixing with a fourth generation neutrino. From an analysis of the partial widths of tau lepton decays we obtain the following bounds at the 90% confidence…

High Energy Physics - Phenomenology · Physics 2007-05-23 John Swain , Lucas Taylor

A measurement of the top-quark mass ($m_t$) in the $t\bar{t}\rightarrow~\textrm{lepton}+\textrm{jets}$ channel is presented, with an experimental technique which exploits semileptonic decays of $b$-hadrons produced in the top-quark decay…

High Energy Physics - Experiment · Physics 2023-07-10 ATLAS Collaboration

Analytic formulae are given for order alpha_s perturbative QCD corrections to the double differential distribution of the tau lepton energy and the invariant mass of the tau + antineutrino system in semileptonic decays of the bottom quark.…

High Energy Physics - Phenomenology · Physics 2009-10-30 Marek Jezabek , Leszek Motyka

Supersymmetry is perhaps most effectively probed at the Tevatron through production and decay of weak gauginos. Most of the analyses of weak gaugino observables require electrons or muons in the final state. However, it is possible that the…

High Energy Physics - Phenomenology · Physics 2009-10-31 James D. Wells

Recently we have proposed mechanisms to explain origins of the charged lepton spectrum as well as Koide's mass formula, on the basis of U(3)\times O(3) family gauge symmetry. In this note, we review the basic ideas of these mechanisms.…

High Energy Physics - Phenomenology · Physics 2016-04-26 Y. Sumino

We use a new compilation of the hadronic $R$-ratio from available data for the process $e^+e^-\to$ hadrons below the charm mass to determine the strong coupling $\alpha_s$, using finite-energy sum rules. Quoting our results at the $\tau$…

High Energy Physics - Phenomenology · Physics 2018-11-06 Diogo Boito , Maarten Golterman , Alex Keshavarzi , Kim Maltman , Daisuke Nomura , Santiago Peris , Thomas Teubner

The tau -> mu nu nu branching ratio has been measured using data collected from 1990 to 1995 by the OPAL detector at the LEP collider. The resulting value of B(tau->mu nu nu) = 0.1734 +/- 0.0009(stat) +/- 0.0005(syst) has been used in…

High Energy Physics - Experiment · Physics 2009-11-07 L. Kormos
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