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Related papers: Triple seesaw mechanism

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Differently from the canonical seesaw mechanism, which is grounded in grand unified theories, the inverse seesaw mechanism lacks a special framework that realizes it naturally. In this work we advocate that the 3-3-1 model with right-handed…

High Energy Physics - Phenomenology · Physics 2013-05-30 A. G. Dias , C. A. de S. Pires , P. S. Rodrigues da Silva , A. Sampieri

A natural extension of the standard $SU(2)_{\rm L} \times U(1)_{\rm Y}$ gauge model to accommodate massive neutrinos is to introduce one Higgs triplet and three right-handed Majorana neutrinos, leading to a $6\times 6$ neutrino mass matrix…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei Chao , Shu Luo , Zhi-zhong Xing , Shun Zhou

The seesaw and leptogenesis commonly depend on the masses of same particles, and thus are both realized at the same scale. In this work, we demonstrate a new possibility to realize a TeV-scale neutrino seesaw and a natural high-scale…

High Energy Physics - Phenomenology · Physics 2019-01-23 Pei-Hong Gu , Hong-Jian He

We study the possibility to test the Type I seesaw mechanism for neutrino masses at the CERN Large Hadron Collider. The inclusion of three generations of right-handed neutrinos (N_i) provides an attractive option of gauging the B-L…

High Energy Physics - Phenomenology · Physics 2009-10-29 Pavel Fileviez Perez , Tao Han , Tong Li

A natural extension of the standard model to accommodate massive neutrinos is to introduce one Higgs triplet and three right-handed Majorana neutrinos, leading to a 6 \times6 neutrino mass matrix. We show that three light Majorana neutrinos…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei Chao , Shu Luo , Zhi-zhong Xing , Shun Zhou

The inverse seesaw mechanism of neutrino mass, i.e. m_nu = (m_D^2/m_N^2)epsilon_L where epsilon_L is small, is discussed in the context of the U(1)_Sigma model. This is a gauge extension of the Standard Model of particle interactions with…

High Energy Physics - Phenomenology · Physics 2009-11-05 Ernest Ma

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 propose a low energy extension of the Standard Model consisting of an additional gauged $U(1)_{B-L}$ plus three right-handed neutrinos. The lightest right-handed neutrinos have TeV scale masses and may be produced at colliders via their…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. F. King , T. Yanagida

We propose a $B-L$ gauged extension of the Standard Model where light neutrino masses arise from type III seesaw mechanism. Unlike the minimal $B-L$ model with three right handed neutrinos having unit lepton number each, the model with…

High Energy Physics - Phenomenology · Physics 2020-03-24 Anirban Biswas , Debasish Borah , Dibyendu Nanda

Little Higgs models are formulated as effective theories with a cut-off of up to 100 times the electroweak scale. Neutrino masses are then a puzzle, since the usual see-saw mechanism involves a much higher scale that would introduce…

High Energy Physics - Phenomenology · Physics 2009-11-11 F. del Aguila , M. Masip , J. L. Padilla

Knowledge of the mechanism of neutrino mass generation would help understand a lot more about Lepton Number Violation (LNV), the cosmological evolution of the Universe, or the evolu tion of astronomical objects. Here we propose a verifiable…

High Energy Physics - Phenomenology · Physics 2020-03-18 Claudio Dib , Sergey Kovalenko , Ivan Schmidt , Adam Smetana

In pursuit of a balance between theoretical naturalness and experimental testability, we propose two classes of multiple seesaw mechanisms at the TeV scale to understand the origin of tiny neutrino masses. They are novel extensions of the…

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

The Type I, II and hybrid (I+II) seesaw mechanism, which explain why neutrinos are especially light, are consequences of the left-right symmetric model (LRSM). They can be classified by the ranges of parameters of LRSM. We show that a…

High Energy Physics - Phenomenology · Physics 2009-03-04 M. J. Luo , Q. Y. Liu

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

In contrast to the original type I seesaw mechanism that requires right-handed Majorana neutrinos at energies much higher than the electroweak scale, the so-called low scale seesaw models allow lighter masses for the additional neutrinos.…

High Energy Physics - Phenomenology · Physics 2020-02-11 A. E. Cárcamo Hernández , Marcela González , Nicolás A. Neill

In this study, we implement the type-II seesaw mechanism for Dirac neutrino masses within the framework of a 3-3-1 model. To this end, we introduce a scalar sextet and impose both lepton number conservation and invariance under a discrete…

High Energy Physics - Phenomenology · Physics 2025-06-06 Vinícius Oliveira , Patricio Escalona , Lucia Angel , C. A. de S. Pires , Farinaldo S. Queiroz

We propose a modified version of the TeV scale B-L extension of the standard model, where neutrino masses are generated through the inverse seesaw mechanism. We show that heavy neutrinos associated with this model can be accessible via…

High Energy Physics - Phenomenology · Physics 2013-05-29 Shaaban Khalil

We consider the phenomenology of the gauged abelian symmetry B + 3 (L_e - L_mu - L_tau). Right-handed neutrinos necessary to cancel triangle anomalies are used in a type-I seesaw scheme to create active neutrino masses. Breaking the B + 3…

High Energy Physics - Phenomenology · Physics 2012-06-28 Julian Heeck , Werner Rodejohann

In this talk we show how a natural neutrino mass hierarchy can follow from the type I see-saw mechanism, and a natural neutrino mass degeneracy from the type II see-saw mechanism, where the bi-large mixing angles can arise from either the…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. F. King

The see-saw mechanism is usually applied to explain the lightness of neutrinos. The traditional see-saw mechanism introduces at least two right-handed neutrinos for the realistic neutrino spectrum. In the case of supersymmetry, loop…

High Energy Physics - Phenomenology · Physics 2014-12-01 Yi-Lei Tang