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Related papers: Dirac Leptogenesis in Left-Right Symmetric Models

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We propose a unified explanation for the origin of dark matter and baryon number asymmetry on the basis of a non-supersymmetric model for neutrino masses. Neutrino masses are generated in two distinct ways, that is, a tree-level seesaw…

High Energy Physics - Phenomenology · Physics 2008-11-26 Daijiro Suematsu

The paper suggests a left-right mirror symmetric model with the flavor symmetries $Z_{3L}\otimes Z_{3R}$. It can simultaneously accommodate the standard model, neutrino physics and the baryon asymmetry. The fermion masses and $CP$ violation…

High Energy Physics - Phenomenology · Physics 2015-09-15 Wei-Min Yang

The family of Dirac Seesaw models offers an intriguing alternative explanation for the smallness of neutrino masses without necessarily requiring microscopic lepton number violation, when compared to the more familiar class of Majorana…

High Energy Physics - Phenomenology · Physics 2024-01-17 Maximilian Berbig

The left-right symmetric model with doublet and bi-doublet Higgs scalars can accommodate linear, inverse or double seesaw for generating small neutrino masses in the presence of three singlet fermions. If the singlet fermions have small…

High Energy Physics - Phenomenology · Physics 2010-10-29 Pei-Hong Gu , Utpal Sarkar

In the baryogenesis via leptogenesis framework the baryonic asymmetry depends on lepton mass matrices. In a previous paper we used SO(10)-inspired mass matrices and we found few possibilities to obtain a sufficient level of asymmetry. In…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Falcone , F. Tramontano

It is well-known that leptogenesis in low energy scale is difficult in the conventional Type-I seesaw mechanism with hierarchical right-handed neutrino masses. We show that in a class of two Higgs doublet model, where one Higgs doublet…

High Energy Physics - Phenomenology · Physics 2011-07-03 Naoyuki Haba , Osamu Seto

Inspired by the S.M.A.S.H. framework we construct a model that addresses the strong CP problem, axion dark matter, inflation and Dirac neutrino masses as well as leptogenesis. The model possesses only two dynamical scales, namely the SM…

High Energy Physics - Phenomenology · Physics 2022-11-21 Maximilian Berbig

A simplified but very instructive analysis of the seesaw mechanism is here performed. Assuming a nearly diagonal Dirac neutrino mass matrix, we study the forms of the Majorana mass matrix of right-handed neutrinos, which reproduce the…

High Energy Physics - Phenomenology · Physics 2009-11-07 D. Falcone

In many extensions of the Standard Model, including a broad class of left-right symmetric and Grand Unified theories, the light neutrino mass matrix is given by the left-right symmetric seesaw formula $M_\nu = f v_L - \frac{v^2}{v_R} Y_\nu…

High Energy Physics - Phenomenology · Physics 2009-11-11 Pierre Hosteins , Stephane Lavignac , Carlos A. Savoy

We present a simple extension of the Standard Model with three right-handed neutrinos in a SUSY framework, with an additional U(1$)_\text{F}$ abelian flavor symmetry with a non standard leptonic charge $L_e-L_\mu-L_\tau$ for lepton doublets…

High Energy Physics - Phenomenology · Physics 2023-03-01 Giorgio Arcadi , Simone Marciano , Davide Meloni

We discuss leptogenesis constraints on the mass of the right-handed $W$-boson ($W_R$) in a TeV-scale Left-Right seesaw model (LRSM) for neutrino masses. For generic Dirac mass of the neutrinos, i.e. with all Yukawa couplings $\lesssim…

High Energy Physics - Phenomenology · Physics 2014-11-19 P. S. Bhupal Dev , Chang-Hun Lee , R. N. Mohapatra

An extension of the Standard Model (SM) is studied in which two right-handed (RH) neutrinos per generation are incorporated, but considering the hypothesis of the symmetry of lepton and quark contents in order to deprive the number of RH…

High Energy Physics - Phenomenology · Physics 2015-01-13 Ernesto A. Matute

Instead of creating the observed baryon asymmetry of the universe by the decay of right-handed (RH) neutrinos to left-handed leptons, we propose to generate it dominantly by the decay of the RH neutrinos to RH leptons. This mechanism turns…

High Energy Physics - Phenomenology · Physics 2009-11-11 Michele Frigerio , Thomas Hambye , Ernest Ma

We consider left-right symmetric model with spontaneous CP-violation. The Lagrangian of this model is CP invariant and the Yukawa couplings are real. Due to spontaneous breaking of the gauge symmetry, some of the neutral Higgses acquire…

High Energy Physics - Phenomenology · Physics 2014-11-18 Narendra Sahu , S. Uma Sankar

We consider a mirror world scenario, in which light Dirac neutrinos are generated from a seesaw mechanism and leptogenesis occurs at high scale without violating lepton number. After leptogenesis, the conservation laws of the theory imply…

High Energy Physics - Phenomenology · Physics 2020-03-24 Kevin Earl , Chee Sheng Fong , Thomas Gregoire , Alberto Tonero

Our present work explores the possibility of neutrino mass generation through {\em Type-I see-saw} mechanism and provides an explanation of the baryon asymmetry of the Universe via thermal leptogenesis in the framework of $Z_3$-symmetric…

High Energy Physics - Phenomenology · Physics 2020-09-08 Indrani Chakraborty , Himadri Roy

An SO(10) grand unified model considered previously by the authors featuring lopsided down quark and charged lepton mass matrices is successfully predictive and requires that the lightest two right-handed Majorana neutrinons be nearly…

High Energy Physics - Phenomenology · Physics 2011-05-12 Carl H. Albright , S. M. Barr

The minimal gauged U(1)$_{L_\mu-L_\tau}$ model is a simple extension of the Standard Model and has a strong predictive power for the neutrino sector. In particular, the mass spectrum and couplings of heavy right-handed neutrinos are…

High Energy Physics - Phenomenology · Physics 2020-11-25 Kento Asai , Koichi Hamaguchi , Natsumi Nagata , Shih-Yen Tseng

We propose an alternative formulation of a Left-Right Symmetric Model (LRSM) where the difference between baryon number ($B$) and lepton number ($L$) remains an unbroken symmetry. This is unlike the conventional formulation, where $B-L$ is…

High Energy Physics - Phenomenology · Physics 2019-08-21 Patrick D. Bolton , Frank F. Deppisch , Chandan Hati , Sudhanwa Patra , Utpal Sarkar

We provide the first systematic study of the viable parameter space for leptogenesis in the type-I seesaw model with three right-handed neutrinos whose Majorana masses lie below the electroweak scale. We highlight the very rich…

High Energy Physics - Phenomenology · Physics 2019-05-01 Michele Lucente , Asmaa Abada , Giorgio Arcadi , Valerie Domcke , Marco Drewes , Juraj Klaric