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We present a detailed discussion on neutrinoless double beta decay within a class of left-right symmetric models where neutrino mass originates by natural type-II seesaw dominance. The spontaneous symmetry breaking is implemented with…

High Energy Physics - Phenomenology · Physics 2016-11-23 Prativa Pritimita , Nitali Dash , Sudhanwa Patra

We propose a model which uses the seesaw mechanism and the lepton number $\bar L = L_e - L_\mu - L_\tau$ to achieve the neutrino mass spectrum $m_1 = m_2$ and $m_3 = 0$, together with a lepton mixing matrix $U$ with $U_{e3} = 0$. In this…

High Energy Physics - Phenomenology · Physics 2009-10-31 W. Grimus , L. Lavoura

We propose a lepton seesaw model to get the same mass-origin of charged-leptons and neutrinos introducing a modular $A_4$ symmetry. In this scenario, the mass matrix of charged-leptons is induced via seesaw-like mechanism while the mass…

High Energy Physics - Phenomenology · Physics 2026-04-02 Takaaki Nomura , Hiroshi Okada

We consider the Standard Model with right-handed neutrinos to explain the masses of active neutrinos by the seesaw mechanism. Since active neutrinos as well as heavy neutral leptons are Majorana fermions in this case, the lepton number…

High Energy Physics - Phenomenology · Physics 2016-01-15 Takehiko Asaka , Takanao Tsuyuki

We discuss a GUT realization of the supersymmetric triplet seesaw mechanism(recently proposed by us in hep-ph/0604083 and further analyzed in hep-ph/0607298) where the exchange of the heavy triplet states generates both neutrino masses and…

High Energy Physics - Phenomenology · Physics 2008-11-26 Filipe R. Joaquim , Anna Rossi

In the type-I seesaw mechanism, both the light Majorana neutrinos (\nu_1, \nu_2, \nu_3) and the heavy Majorana neutrinos (N_1, ..., N_n) can mediate the neutrinoless double-beta (0\nu\beta\beta) decay. We point out that the contribution of…

High Energy Physics - Phenomenology · Physics 2009-09-28 Zhi-zhong Xing

Current experimental data allow the zero value for one neutrino mass, either m_1 =0 or m_3 =0. This observation implies that a realistic neutrino mass texture can be established by starting from the limit (a) m_1 = m_2 =0 and m_3 \neq 0 or…

High Energy Physics - Phenomenology · Physics 2008-11-26 Shu Luo , Zhi-zhong Xing

We consider the TeV scale left-right symmetric theory which can accommodate low scale seesaw mechanisms consistent with neutrino oscillation data and find new physics contributions to neutrinoless double beta decay. The model facilitates…

High Energy Physics - Phenomenology · Physics 2016-12-26 Prativa Pritimita , Nitali Dash , Sudhanwa Patra

The pursuit for the genuine fundamental description, governing nature at some high-energy scale, must invariably consider the yet-unknown mechanism behind the generation of neutrino mass. Lepton-flavor violating decays $l_\alpha\to…

High Energy Physics - Phenomenology · Physics 2025-04-03 Adrián González-Quiterio , Héctor Novales-Sánchez

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 study LHC signatures of Type III seesaw in which SU(2)_L triplet leptons are introduced to supply the heavy seesaw masses. To detect the signals of these heavy triplet leptons, one needs to understand their decays to standard model…

High Energy Physics - Phenomenology · Physics 2010-01-08 Tong Li , Xiao-Gang He

Neutrinos stand out among elementary particles through their unusually small masses. Various seesaw mechanisms attempt to explain this fact. In this work applying insights from matrix theory we are in a position to treat variants of seesaw…

High Energy Physics - Phenomenology · Physics 2020-09-04 Wojciech Flieger , Janusz Gluza

In the type-II seesaw mechanism, the neutrino mass generation could be tested experimentally if the Higgs triplet is at the TeV scale and has a small cubic coupling to the standard model Higgs doublet. We show such small triplet-doublet…

High Energy Physics - Phenomenology · Physics 2020-01-15 Pei-Hong Gu

We present a Froggatt-Nielsen flavor model that yields a minimal realization of the type-I seesaw mechanism. This seesaw model is minimal for three reasons: (i) It features only two rather than three right-handed sterile neutrinos: N_1 and…

High Energy Physics - Phenomenology · Physics 2016-12-30 Thomas Rink , Kai Schmitz , Tsutomu T. Yanagida

We consider a model of neutrino mass with a scalar triplet $(\xi^{++},\xi^+,\xi^0)$ assigned lepton number $L=0$, so that the tree-level Yukawa coupling $\xi^0 \nu_i \nu_j$ is not allowed. It is generated instead through the interaction of…

High Energy Physics - Phenomenology · Physics 2016-02-01 Sean Fraser , Corey Kownacki , Ernest Ma , Oleg Popov

We study the search potential of heavy triplet leptons in Type III Seesaw mechanism at future high-energy and high-luminosity muon colliders. The impact of up-to-date neutrino oscillation results is taken into account on neutrino parameters…

High Energy Physics - Phenomenology · Physics 2022-09-27 Tong Li , Han Qin , Chang-Yuan Yao , Man Yuan

We review the main features and results of thermal leptogenesis within the type I seesaw mechanism, the minimal extension of the Standard Model explaining neutrino masses and mixing. After presenting the simplest approach, the vanilla…

High Energy Physics - Phenomenology · Physics 2015-06-12 Steve Blanchet , Pasquale Di Bari

Parametrization of the neutrino mass matrix in terms of well-known measured quantities is an attractive way to obtain a phenomenologically viable form. We propose a model of neutrino mass matrix based on type-II seesaw mechanism adhering…

High Energy Physics - Phenomenology · Physics 2021-02-15 Satyabrata Datta , Ambar Ghosal

In the extension of the standard model with one right-handed neutrino and one Higgs triplet, we propose a suppression mechanism, obtaining small masses for the active neutrinos, while mixing angles are predicted with a right-handed neutrino…

High Energy Physics - Phenomenology · Physics 2018-10-12 R. Martinez , F. Ochoa , M. Ospina

The occurrence of neutrino oscillations demands the existence of flavour violation in charged lepton sector. The relation between the branching ratios of different charged lepton flavour violating (CLFV) decay modes depends on the details…

High Energy Physics - Phenomenology · Physics 2025-03-11 Pravesh Chndra Awasthi , Jai More , Akhila Kumar Pradhan , Kumar Rao , Purushottam Sahu , S. Uma Sankar
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