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Related papers: Charged Lepton Mass Formula -- Development and Pro…

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Charged-lepton-flavor-violation is predicted in several new physics scenarios. We update the analysis of $\tau$ lepton decays into a light charged lepton ($\ell$ = $e^{\pm}$ or $\mu^{\pm}$) and a vector meson ($V^0$ = $\rho^0$, $\phi$,…

High Energy Physics - Experiment · Physics 2023-06-26 Belle Collaboration , N. Tsuzuki , K. Inami , I. Adachi , H. Aihara , D. M. Asner , H. Atmacan , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , P. Behera , K. Belous , J. Bennett , M. Bessner , B. Bhuyan , T. Bilka , D. Biswas , D. Bodrov , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , M. Campajola , D. Červenkov , M. -C. Chang , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -J. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , J. Cochran , S. Das , N. Dash , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , Z. Doležal , T. V. Dong , D. Dossett , S. Dubey , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , V. Gaur , A. Giri , P. Goldenzweig , Y. Guan , K. Gudkova , X. Han , T. Hara , K. Hayasaka , H. Hayashii , M. T. Hedges , D. Herrmann , W. -S. Hou , C. -L. Hsu , T. Iijima , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , E. -J. Jang , S. Jia , Y. Jin , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , K. Kinoshita , P. Kodyš , T. Konno , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , M. Kumar , K. Kumara , A. Kuzmin , Y. -J. Kwon , S. C. Lee , J. Li , L. K. Li , Y. Li , J. Libby , K. Lieret , Y. -R. Lin , D. Liventsev , Y. Ma , A. Martini , M. Masuda , K. Matsuoka , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , K. Miyabayashi , R. Mizuk , G. B. Mohanty , M. Nakao , Z. Natkaniec , A. Natochii , L. Nayak , M. Niiyama , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , P. Oskin , G. Pakhlova , T. Pang , S. Pardi , H. Park , J. Park , S. -H. Park , A. Passeri , S. Paul , T. K. Pedlar , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , A. Rostomyan , N. Rout , G. Russo , S. Sandilya , A. Sangal , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , M. E. Sevior , W. Shan , M. Shapkin , C. Sharma , J. -G. Shiu , E. Solovieva , M. Starič , M. Sumihama , T. Sumiyoshi , M. Takizawa , U. Tamponi , K. Tanida , F. Tenchini , M. Uchida , T. Uglov , Y. Unno , S. Uno , P. Urquijo , Y. Ushiroda , S. E. Vahsen , G. Varner , A. Vinokurova , D. Wang , E. Wang , M. -Z. Wang , X. L. Wang , S. Watanuki , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , J. Yelton , Y. Yook , L. Yuan , Y. Zhai , V. Zhilich , V. Zhukova

We present selected new results on leptonic B meson decays from the BaBar experiment: searches for the decays B0->l+l-, B+->l+nu and B0->l+tau-, and B->Knunubar, where l=e or mu. The decay modes imply also their charge conjugations. We…

High Energy Physics - Experiment · Physics 2008-05-16 Kim Hojeong

A new flipped $SU(3)_C\otimes SU(4)_L\otimes U(1)_X$ model without exotic electric charges is proposed. All the quarks families are arranged in the same representation while leptons generations are in different representations leading to a…

High Energy Physics - Phenomenology · Physics 2021-07-19 Meriem Djouala , Noureddine Mebarki , Habib Aissaoui

In this paper we present a connection between the results obtained from a semiclassical study of a relativistic, two-body system, and the leptons masses. Some possible consequences are also discussed.

Nuclear Theory · Physics 2008-10-06 I. V. Grossu , C. Besliu

Very little is known about the mass spectrum of fermions in the standard model. In this talk, I point out that in the simplest extension of the standard model, in which all right-handed fields are singlets, it is quite possible that a…

High Energy Physics - Phenomenology · Physics 2007-05-23 Marc Sher

We explore alternative descriptions of the charged lepton sector in modular invariant models of lepton masses and mixing angles. In addition to the modulus, the symmetry breaking sector of our models includes ordinary flavons. Neutrino mass…

High Energy Physics - Phenomenology · Physics 2020-03-18 Juan Carlos Criado , Ferruccio Feruglio , Simon J. D. King

Traditional analysis of $g=2(1+\kappa )$ experiments for charged leptons use a classical spin vector picture. For muons, we here employ a more exact Dirac quantum four component spinor theory. Survival probabilities (including wave packet…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. Widom , Y. N. Srivastava

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

The decay rate of the $\tau$ lepton into hadrons of invariant mass smaller than $Q\gg\Lambda_{\rm QCD}$ can be calculated in QCD using the OPE. Using experimental data on the hadronic mass distribution, the running coupling constant…

High Energy Physics - Phenomenology · Physics 2007-05-23 Maria Girone , Matthias Neubert

Including contributions of scale-dependent vacuum expectation values, we derive new analytic formulas and obtain substantially different numerical predictions for the running masses of quarks and charged-leptons at higher scales in the SM,…

High Energy Physics - Phenomenology · Physics 2008-11-26 C. R. Das , M. K. Parida

For a resonance decaying to $\tau^+\tau^-$, it is difficult to reconstruct its mass accurately because of the presence of neutrinos in the decay products of the $\tau$ leptons. If the resonance is heavy enough, we show that its mass can be…

High Energy Physics - Experiment · Physics 2016-08-09 Li-Gang Xia

Recently, the L3 collaboration has reported the observation of four events in the reactions e+ e- --> L+ L- + (2 Photons), L = e, mu, tau, with the invariant photon pair mass near 60 GeV in a data sample collected in the L3 detector…

High Energy Physics - Phenomenology · Physics 2009-12-30 S. Jadach , B. F. L. Ward , S. A. Yost

The branching fractions of $\tau$ lepton decays with the production of strange scalar mesons both in the ground and first radially excited states $\tau \to \nu_\tau [K^*_0(700), K^*_0(1430)]$ and $\tau \to \nu_\tau [K^*_0(700)\pi,…

High Energy Physics - Phenomenology · Physics 2023-03-22 Mikhail K. Volkov , K. Nurlan

We present a flavor model with the $S_3$ modular invariance in the framework of SU(5) GUT. The $S_3$ modular forms of weights $2$ and $4$ give the quark and lepton mass matrices with a common complex parameter, the modulus $\tau$. The GUT…

High Energy Physics - Phenomenology · Physics 2020-05-27 Tatsuo Kobayashi , Yusuke Shimizu , Kenta Takagi , Morimitsu Tanimoto , Takuya H. Tatsuishi

This White Paper outlines a proposal for an upgraded forward region to extend CMS lepton (e, mu) and photon physics reach out to 2.2<eta<5 for LHC and SLHC, which also provides better performance for the existing or new forward hadron…

Instrumentation and Detectors · Physics 2013-08-27 Burak Bilki , Lucien Cremaldi , Yasar Onel , David R. Winn , Taylan Yetkin

Form factors parameterizing radiative leptonic decays of heavy mesons $% (B^{+}\to \gamma l^{+}\nu_{l}) $ for photon energy are computed in the language of dispersion relation. The contributing states to the absorptive part in the…

High Energy Physics - Phenomenology · Physics 2011-09-13 Mariam Saleh Khan , M. Jamil Aslam , Amjad Hussain Shah Gilani , Riazuddin

Radiative muon and tau lepton decays are described within the model-independent approach with the help of generalized Michel parameters. The exact dependence on charged lepton masses is taken into account. The results are relevant for…

High Energy Physics - Phenomenology · Physics 2016-10-12 A. B. Arbuzov , T. V. Kopylova

One of purposes for High Energy accelerator experiments is confrontation of theory and measurements in ever new realms. Any new agreement extends theory applicability domain, any discrepancy hints to unexplained. That calls for better…

High Energy Physics - Phenomenology · Physics 2025-07-23 Z. Was

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 masses of quarks and leptons in units of $m_t$ are expressed in powers of $\sigma=\sqrt{m_c/m_t}$. The regularities found suggest specific mass matrices. They reproduce all masses and mixings in striking agreement with observation. A 90…

High Energy Physics - Phenomenology · Physics 2016-09-06 Berthold Stech