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Related papers: An Alternative to See-Saw

200 papers

In the supersymmetric left-right model, the light neutrino masses are given by the Type-II seesaw mechanism. A duality property about this mechanism indicates that there exist eight possible Higgs triplet Yukawa couplings which result in…

High Energy Physics - Phenomenology · Physics 2015-05-13 Wei Chao

We systematically construct realistic mass matrices for the type-I seesaw mechanism out of more than 20 trillion possibilities. We use only very generic assumptions from extended quark-lepton complementarity, i.e., the leptonic mixing…

High Energy Physics - Phenomenology · Physics 2008-11-26 Florian Plentinger , Gerhart Seidl , Walter Winter

We show that the assumption of type II seesaw mechanism for small neutrino masses coupled with $b-\tau$ mass unification in a minimal SUSY SO(10) model leads not only to a natural understanding of large atmospheric mixing angle…

High Energy Physics - Phenomenology · Physics 2008-11-26 H. S. Goh , R. N. Mohapatra , Siew-Phang Ng

A novel scenario is presented within the Type-I seesaw mechanism in which no other beyond Standard Model fields except three heavy right handed neutrinos, have been considered. Light neutrino masses around sub eV scale, could be possible at…

High Energy Physics - Phenomenology · Physics 2024-11-26 Kunal Pandey , Rathin Adhikari

We propose a model for leptons based on the smallest modular finite group $\Gamma_2\cong S_3$ that, for the first time, accounts for both the hints of large low-energy CP-violation in the lepton sector and the matter-antimatter asymmetry of…

High Energy Physics - Phenomenology · Physics 2024-05-09 Simone Marciano , Davide Meloni , Matteo Parriciatu

We propose a scheme in that the masses of the heavier leptons obey seesaw type relations. The light lepton masses, except the electron and the electron neutrino ones are generated by one loop level radiative corrections. We work in a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Nelson V. Cortez , Mauro D. Tonasse

In left-right symmetric models (LRSM) the light neutrino masses arise from two sources: the seesaw mechanism and a VEV of an SU(2)$_L$ triplet. If the left-right symmetry breaking, $v_R$, is low, $v_R\lsim15\TeV$, the contributions to the…

High Energy Physics - Phenomenology · Physics 2009-11-07 Oleg Khasanov , Gilad Perez

We suggest a hybrid seesaw model where relatively ``light''right-handed neutrinos give no contribution to the neutrino mass matrix due to a special symmetry. This allows their Yukawa couplings to the standard model particles to be…

High Energy Physics - Phenomenology · Physics 2009-04-29 Pei-Hong Gu , M. Hirsch , Utpal Sarkar , J. W. F. Valle

The seesaw mechanism for neutrino masses is introduced and some of its different realizations and applications are discussed. It is pointed out how they can be used to understand the bi-large mixing patterns among neutrinos in combination…

High Energy Physics - Phenomenology · Physics 2017-08-23 R. N. Mohapatra

We make a general analysis of neutrino phenomenology for the case neutrino masses are generated by the see-saw mechanism with just two right handed neutrinos. We find general constraints on leptogenesis and lepton flavour violating…

High Energy Physics - Phenomenology · Physics 2009-11-10 A. Ibarra , G. G. Ross

We study the Zee model in the framework of the split fermion model in $M_4\times S_1/Z_2$ spacetime. Neutrino masses are generated through 1-loop diagrams without the right-handed neutrinos introduced. By assuming an order one anarchical…

High Energy Physics - Phenomenology · Physics 2011-02-15 We-Fu Chang , I-Ting Chen , Siao-Cing Liou

The seesaw mechanism is attractive not only because it "explains'' small neutrino mass, but also because of its packaging with the SUSY-GUT, leptogenesis, Dark Matter, and electroweak symmetry breaking. However, this package has the flavor,…

High Energy Physics - Phenomenology · Physics 2009-09-29 Hitoshi Murayama

In this paper, we explore a new avenue to a natural explanation of the observed tiny neutrino masses with a dynamical realization of the three-generation structure in the neutrino sector. Under the magnetized background based on $T^2/Z_2$,…

High Energy Physics - Phenomenology · Physics 2018-07-24 Makoto Ishida , Kenji Nishiwaki , Yoshiyuki Tatsuta

We discuss what kinds of combinations of Yukawa interactions can generate the Majorana neutrino mass matrix. We concentrate on the flavor structure of the neutrino mass matrix because it does not depend on details of the models except for…

High Energy Physics - Phenomenology · Physics 2016-01-20 Shinya Kanemura , Hiroaki Sugiyama

The problem of testing leptogenesis from low energy experiments is discussed following three different perspectives. Firstly, we review the prospects that from low energy experiments we could reconstruct the neutrino Yukawa coupling matrix…

High Energy Physics - Phenomenology · Physics 2007-05-23 Thomas Hambye

We consider the problem of neutrino masses and mixing within the general framework of standard (type-I) seesaw models leading to three light neutrinos. Under the assumption of a hierarchical neutrino mass spectrum \lambda^4: \lambda : 1,…

High Energy Physics - Phenomenology · Physics 2013-05-30 M. Paraskevas , K. Tamvakis

Seesaw models with a slightly broken lepton number symmetry can explain small neutrino masses, and allow for low-scale leptogenesis. We make a thorough analysis of leptogenesis within the simplest model with two right-handed (RH) neutrinos…

High Energy Physics - Phenomenology · Physics 2010-04-21 Takehiko Asaka , Steve Blanchet

We present a $SU(5)\times U(1)_F$ supersymmetric model for neutrino masses and mixings that implements the seesaw mechanism by means of the heavy SU(2) singlets and triplets states contained in three adjoints of SU(5). We discuss how…

High Energy Physics - Phenomenology · Physics 2015-05-30 Enrico Nardi , Diego Restrepo , Mauricio Velasquez

We discuss the prospects for detecting right-handed neutrinos which are introduced in the see-saw mechanism at future colliders. This requires a very accurate cancellation between contributions from different right-handed neutrinos to the…

High Energy Physics - Phenomenology · Physics 2011-11-10 Joern Kersten

A Higgs sextet is introduced in order to generate Dirac and Majorana neutrino masses in the 331 model with right-handed neutrinos. As will be seen, the present sextet introduction leads to a rich neutrino mass structure. The smallness of…

High Energy Physics - Phenomenology · Physics 2009-11-11 Nguyen Anh Ky , Nguyen Thi Hong Van