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Related papers: A Timeon Model of Quark and Lepton Mass Matrices

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We explore the possibility of having a successful leptogenesis through oscillations between new sterile fermion states added to the Standard Model field content in a well motivated framework, naturally giving rise to the required mass…

High Energy Physics - Phenomenology · Physics 2017-08-31 Asmaa Abada , Giorgio Arcadi , Valerie Domcke , Michele Lucente

One of the key assumptions of the Standard Model of fundamental particles is that the interactions of the charged leptons, namely electrons, muons, and taus, differ only because of their different masses. While precision tests comparing…

High Energy Physics - Experiment · Physics 2023-03-03 Gregory Ciezarek , Manuel Franco Sevilla , P. M. Hamilton , Robert Kowalewski , Thomas Kuhr , Vera Lüth , Yutaro Sato

Forces beyond those of the standard model may manifest themselves at low energies as four-fermion contact interactions. If these new forces are independent of colour and flavour quantum numbers including baryon and lepton number, then all…

High Energy Physics - Phenomenology · Physics 2009-10-30 Wilfried Buchmuller , Daniel Wyler

We present a class of supersymmetric models with complete generations of composite quarks and leptons using recent non-perturbative results for the low energy dynamics of supersymmetric QCD. In these models, the quarks arise as composite…

High Energy Physics - Phenomenology · Physics 2009-10-30 Markus A. Luty , Rabindra N. Mohapatra

A generic search for anomalous production of events with at least three charged leptons is presented. The data sample consists of $pp$ collisions at $\sqrt{s}=8$ TeV collected in 2012 by the ATLAS experiment at the CERN Large Hadron…

High Energy Physics - Experiment · Physics 2015-09-16 ATLAS Collaboration

We demonstrate that in a recently proposed unified leptoquark model based on the gauge group $SU(4)_C\times SU(2)_L \times U(1)_R$ significant deviations from the Standard Model values of $R_K$ and $R_{K^*}$ can be accommodated without any…

High Energy Physics - Phenomenology · Physics 2021-01-07 Thomas Faber , Matěj Hudec , Helena Kolešová , Yang Liu , Michal Malinský , Werner Porod , Florian Staub

We examine an effective field theory inspired by Little Flavor that demonstrates a new paradigm for generating quark and lepton masses in which the scale of new flavor physics can be at the few TeV level, and new $Z'$ and $W'$ bosons are…

High Energy Physics - Phenomenology · Physics 2015-09-29 Dorota M. Grabowska , David B. Kaplan

We propose a model based on the gauge group $SU(3)_{C}\otimes SU(3)_{L}\otimes U(1)_{X}$ with an extra $S_{3}$ flavor symmetry, which accounts for the lepton masses and mixing. The small active neutrino masses are generated via a double…

High Energy Physics - Phenomenology · Physics 2014-10-15 A. E. Cárcamo Hernández , E. Cataño Mur , R. Martinez

We study supersymmetric extra U(1) model with $S_4$ flavor symmetry. The flavor symmetry not only stabilizes proton but also suppresses the flavor changing processes without raising the supersymmetry breaking scale. After the flavor…

High Energy Physics - Phenomenology · Physics 2020-12-01 Yasuhiro Daikoku , Hiroshi Okada

We show that the observed structure of quark and lepton masses and mixing angles can arise entirely geometrically from superstring constructions, at the renormalizable level. The model we consider is a $Z_3$ orbifold compactification of…

High Energy Physics - Phenomenology · Physics 2009-11-07 S. A. Abel , C. Munoz

The origin of the matter-antimatter asymmetry in the Universe is a fundamental question of physics. Electroweak baryogenesis is a compelling scenario for explaining it but it requires beyond the Standard Model sources of the CP symmetry…

High Energy Physics - Phenomenology · Physics 2021-07-14 J. Alonso-González , L. Merlo , S. Pokorski

We construct a 3-3-1 model based on non-Abelian discrete symmetry $T_7$ responsible for the fermion masses. Neutrinos get masses from only anti-sextets which are in triplets $\underline{3}$ and $\underline{3}^*$ under $T_7$. The flavor…

High Energy Physics - Phenomenology · Physics 2014-04-29 V. V. Vien , H. N. Long

In this work, we have proposed a modular $A_4$ symmetric model of neutrino mass which, simultaneously, explains observed baryon asymmetry of the Universe(BAU). In minimal extension of the standard model(SM) with two right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2021-10-04 Monal Kashav , Surender Verma

We consider the see-saw mechanism for hierarchical Dirac and Majorana neutrino mass matrices m_D and M_R, including the CP violating phases. Simple arguments about the structure of the neutrino mass matrix and the requirement of successful…

High Energy Physics - Phenomenology · Physics 2011-07-19 Werner Rodejohann

In this work, we have modified a scenario, originally proposed by Grimus and Lavoura, in order to obtain maximal values for atmospheric mixing angle and CP violating Dirac phase of the lepton sector. To achieve this, we have employed CP and…

High Energy Physics - Phenomenology · Physics 2022-10-05 Joy Ganguly , Raghavendra Srikanth Hundi

Majorana masses of the neutrino implies lepton number violation and is intimately related to the lepton asymmetry of the universe, which gets related to the baryon asymmetry of the universe in the presence of the sphalerons during the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Utpal Sarkar

We construct a new gauged $U(1)_\ell$ lepton number model which is anomaly-free for each SM generation. The active neutrino masses are radiatively generated with a minimal scalar sector. The phenomenology and collider signals are studied.…

High Energy Physics - Phenomenology · Physics 2018-08-15 We-Fu Chang , John N. Ng

Leptoquark-Higgs interactions induce mixing between leptoquark states with different chiralities once the electro-weak symmetry is broken. In such LQ models Majorana neutrino masses are generated at 1-loop order. Here we calculate the…

High Energy Physics - Phenomenology · Physics 2008-11-26 D. Aristizabal Sierra , M. Hirsch , S. G. Kovalenko

The recent measurement of the reactor angle as $\sin^2 2\theta_{13} = 0.092 \pm 0.016(stat) \pm 0.005(syst)$ come from the Daya Bay collaboration. Evidence of nonzero \theta_{13} was also there at T2K, MINOS and Double Chooz experiments. We…

High Energy Physics - Phenomenology · Physics 2012-05-23 Swarup Kumar Majee

The dipole moments of the leptons and quarks are matrices in flavor space, which can potentially reveal as much about the flavor structure of the theory as do the mass matrices. The off-diagonal elements of the dipole matrices lead to…

High Energy Physics - Phenomenology · Physics 2014-11-17 K. S. Babu , S. M. Barr , Ilja Dorsner