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Related papers: Three generations mixing and the $\tau$ decay puzz…

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We analyze the impact of the data on long baseline \nu_\mu disappearance from the K2K experiment and reactor \bar\nu_e disappearance from the KamLAND experiment on the determination of the leptonic three-generation mixing parameters.…

High Energy Physics - Phenomenology · Physics 2011-01-31 M. C. Gonzalez-Garcia , Carlos Pena-Garay

In the conventional seesaw models of neutrino masses, leptogenesis occurs at a very high scale. Three approaches have been discussed in the literature to lower the scale of leptogenesis: mass degeneracy, hierarchy of couplings and…

High Energy Physics - Phenomenology · Physics 2010-11-15 Pei-Hong Gu , Utpal Sarkar

We discussed the impact of the existence of B -> D' l nu decays to radially excited D' mesons on various long-standing puzzles in the experimental data of semileptonic b -> c ell nu decays, as summarized in our recent article…

High Energy Physics - Phenomenology · Physics 2013-01-21 Florian U. Bernlochner , Zoltan Ligeti , Sascha Turczyk

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

We investigate the consequences of $\mu-\tau$ reflection symmetry in presence of a light sterile neutrino for the $3+1$ neutrino mixing scheme. We discuss the implications of total $\mu-\tau$ reflection symmetry as well partial $\mu-\tau$…

High Energy Physics - Phenomenology · Physics 2019-08-28 Kaustav Chakraborty , Srubabati Goswami , Biswajit Karmakar

Motivated by a recent rather surprising conclusion based on the 1992 PDG data on the pion, kaon and lepton decays that if three generations of neutrinos are assumed to be massive and mixed, the heaviest neutrino, $\nu_3$, could have a mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Bottino , N. Fornengo , C. W. Kim , G. Mignola

The observed quark hierarchies suggest a simple family symmetry. Generalized to leptons through grand-unified quantum numbers, it produces a neutrino mixing matrix with order-one \nu_{\mu} - \nu_{\tau} mixing, and order-\lambda^3 \nu_e -…

High Energy Physics - Phenomenology · Physics 2009-10-31 John K. Elwood , Nikolaos Irges , Pierre Ramond

LHCb reported anomalies in $B\to K^* \mu^+\mu^-$, $B_s\to\phi\mu^+\mu^-$ and $R(K)=B\to K \mu^+\mu^-/B\to K e^+e^-$. Furthermore, BaBar, BELLE and LHCb found hints for the violation of lepton flavour universality violation in…

High Energy Physics - Phenomenology · Physics 2015-11-04 Lorenzo Calibbi , Andreas Crivellin , Toshihiko Ota

Apart from offering explanations not only for the distinctive fermion mass and mixing patterns but also for the actual values of the mass and mixing parameters, the dual colour solution to the generation puzzle gives numerous detailed…

High Energy Physics - Phenomenology · Physics 2007-05-23 HM Chan

We consider the maximal U(3) horizontal scheme as a handle on fermion masses and mixings. In particular, we attempt to explain the large top Yukawa coupling and the masses and mixing in the two heaviest generations. A simple model is…

High Energy Physics - Phenomenology · Physics 2016-08-25 Andrija Rasin

The $\mu\tau$-reflection symmetry is a simple symmetry capable of predicting all the unknown CP phases of the lepton sector and the atmospheric angle but too simple to predict the absolute neutrino mass scale or the mass ordering. We show…

High Energy Physics - Phenomenology · Physics 2017-01-23 C. C. Nishi , B. L. Sánchez-Vega

We study the phenomenology of new heavy vector-like fermions that couple to the third generation quarks via Yukawa interactions, covering all the allowed representations under the standard model gauge groups. We first review tree and loop…

High Energy Physics - Phenomenology · Physics 2010-12-09 Giacomo Cacciapaglia , Aldo Deandrea , Daisuke Harada , Yasuhiro Okada

We discuss the implications for lepton mixing and CP violation of structure in the lepton mass matrices, for the case that neutrino masses are generated by the see-saw mechanism with an hierarchical structure for the Majorana masses. For a…

High Energy Physics - Phenomenology · Physics 2015-06-25 A. Ibarra , G. G. Ross

Charged scalar particles introduced in some extensions of the standard model can induce $\tau$ leptonic decay at tree level. We find that with some charged SU(2)-singlet scalar particles, like ones introduced in Zee-type models, $\tau$…

High Energy Physics - Phenomenology · Physics 2009-10-22 Zhijian Tao

In this paper, the lepton flavor violating $\tau\to \ell P(V)$ ($P,V= \pi^0, \eta, \eta^{\prime}, \rho^0, \omega, \phi$) and $\tau\to 3\ell$ ($\ell = e, \mu$) decays are studied in the framework of the type-III seesaw model, in which new…

High Energy Physics - Phenomenology · Physics 2014-11-18 Abdesslam Arhrib , Rachid Benbrik , Chuan-Hung Chen

The compelling experimental evidences for oscillations of solar and atmospheric neutrinos imply the existence of 3-neutrino mixing in vacuum. We briefly review the phenomenology of 3-neutrino mixing, and the current data on the 3-neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-11 S. T. Petcov

Motivated by the large discrepancy of CP-violating phase in $\bar{B}_s-B_s$ mixing between the experimental data and the Standard Model prediction, we pursue possible solutions within a family non-universal $Z^{\prime}$ model. Within such a…

High Energy Physics - Phenomenology · Physics 2010-03-02 Qin Chang , Xin-Qiang Li , Ya-Dong Yang

We present a model for third-family quark-lepton unification at the TeV scale featuring a composite Higgs sector. The model is based on a variant of the Pati-Salam model, the so-called 4321 model, consisting of the gauge group $SU(4)\times…

High Energy Physics - Phenomenology · Physics 2020-11-25 Javier Fuentes-Martin , Peter Stangl

A novel relation is found which gives the 2-3 lepton mixing angle in terms of quark masses and CKM mixing: \tan\theta_{\mu\tau}=(m_b/m_s)V_{cb}. This relation, which is remarkably in good agreement with the quark data and the large lepton…

High Energy Physics - Phenomenology · Physics 2009-10-31 Masako Bando , Taichiro Kugo , Koichi Yoshioka

Although the measurement of the reactor angle has killed tribimaximal lepton mixing, its descendants survive with charged lepton corrections, or in less constrained forms such as trimaximal mixing and/or mu-tau symmetry, each with…

High Energy Physics - Phenomenology · Physics 2019-05-06 Stephen F King