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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

Seesaw mechanism appears to be the simplest and most appealing way to understand small neutrino masses observed in recent experiments. It introduces three right handed neutrinos with heavy masses to the standard model, with at least one…

High Energy Physics - Phenomenology · Physics 2014-11-18 R. N. Mohapatra

We prove a general low-energy theorem establishing a generic relation between the neutrino Majorana mass and the superpartner sneutrino B-L-violating "Majorana"-like mass term. The theorem states that, if one of these two quantities is…

High Energy Physics - Phenomenology · Physics 2009-10-30 M. Hirsch , H. V. Klapdor-Kleingrothaus , S. G. Kovalenko

We present the first detailed phenomenological analysis of a radiative Majorana neutrino mass model constructed from opening up a $\Delta L = 2$ mass-dimension-11 effective operator constructed out of standard model fields. While three such…

High Energy Physics - Phenomenology · Physics 2020-04-22 John Gargalionis , Iulia Popa-Mateiu , Raymond R. Volkas

A non-minimal approximation for effective masses of light and heavy neutrinos in the framework of a type-I seesaw mechanism with three generations of sterile Majorana neutrinos which recover the symmetry between quarks and leptons is…

High Energy Physics - Phenomenology · Physics 2023-03-14 Mikhail Dubinin , Elena Fedotova

Neutrino masses arise via a seesaw mechanism and its mass hierarchy, with assumption that heavy Majorana neutrino mass matrix subject to $\mu-\tau$ symmetry and invariant under a cyclic permutation, are evaluated. Within this scenario, the…

High Energy Physics - Phenomenology · Physics 2010-06-03 Asan Damanik

The existence of neutrino mass and mixing is a strong pointer towards physics beyond the standard model. An overview of the possibility of having neutrino masses in supersymmetric theories is attempted here. Some of the recent works…

High Energy Physics - Phenomenology · Physics 2007-05-23 Biswarup Mukhopadhyaya

If neutrino masses are realized through the see-saw mechanism, can the right-handed neutrinos be produced and detected at present and future colliders? The answer is negative in the most popular see-saw scenarios for the simple reason that…

High Energy Physics - Phenomenology · Physics 2008-11-26 P. Q. Hung

We examine supersymmetric contributions to transition magnetic moments of Majorana neutrinos. We first give the general formula for it. In concrete evaluations, informations of neutrino mass matrix elements including CP phases are…

High Energy Physics - Phenomenology · Physics 2009-11-10 Takeshi Fukuyama , Tatsuru Kikuchi , Nobuchika Okada

We analyze the spectrum and mixing among neutrinos in the minimal supersymmetric standard model with explicit breaking of R parity. It is shown that ({\em i}) the mixing among neutrinos is naturally large and ({\em ii}) the non zero…

High Energy Physics - Phenomenology · Physics 2009-10-28 Anjan S. Joshipura , Marek Nowakowski

In theories where $B-L$ is a spontaneously broken local symmetry, the cosmological baryon asymmetry can be generated by the out-of-equilibrium decay of heavy Majorana neutrinos. We study this mechanism assuming a similar pattern of mixings…

High Energy Physics - Phenomenology · Physics 2009-10-28 W. Buchmuller , M. Plumacher

We reconsider the possibility that Majorana masses for the three known neutrinos are generated radiatively by the presence of a fourth generation and one right-handed neutrino with Yukawa couplings and a Majorana mass term. We find that the…

High Energy Physics - Phenomenology · Physics 2011-08-01 Alberto Aparici , Juan Herrero-García , Nuria Rius , Arcadi Santamaria

We show that one of the ways of obtaining consistency between the idea of supersymmetric grand unification and an apparent low value of $\alpha_{strong}(M_Z)\simeq .11$ indicated by several low energy experiments is to have an intermediate…

High Energy Physics - Phenomenology · Physics 2009-10-02 Biswajoy Brahmachari , Rabindra N Mohapatra

In SU(3)_L x U(1)_N gauge models for electroweak interactions, we discuss how to implement a radiative mechanism of generating Majorana neutrino masses by considering the property that the Higgs scalar, which has a coupling to a charged…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yutaka Okamoto , Masaki Yasue

The problem of Majorana neutrino mass generated in Arkani-Hamed--Dimopoulos-Dvali model with n extra spatial dimensions is discussed. Taking into account constraints on neutrino masses coming from cosmological observations, it is possible…

High Energy Physics - Phenomenology · Physics 2009-11-10 Marek Gozdz , Wieslaw A. Kaminski

A new idea for neutrino mass was proposed recently, where its smallness is not due to the seesaw mechanism, i.e. not inversely proportional to some large mass scale. It comes from a one-loop mechanism with dark matter in the loop consisting…

High Energy Physics - Phenomenology · Physics 2013-06-06 Subhaditya Bhattacharya , Ernest Ma , Alexander Natale , Ahmed Rashed

We study Majorana neutrino masses induced by D-brane instanton effects in magnetized orbifold models. We classify possible cases, where neutrino masses can be induced. Three and four generations are favored in order to generate neutrino…

High Energy Physics - Theory · Physics 2021-03-15 Kouki Hoshiya , Shota Kikuchi , Tatsuo Kobayashi , Kaito Nasu , Hikaru Uchida , Shohei Uemura

We studied a left-right symmetric model that can accommodate the neutrino dark energy (\nd) proposal. Type III seesaw mechanism is implemented to give masses to the neutrinos. After explaining the model, we study the consistency of the…

High Energy Physics - Phenomenology · Physics 2010-04-21 Jitesh R. Bhatt , Pei-Hong Gu , Utpal Sarkar , Santosh K. Singh

Assuming hierarchical neutrino masses we calculate the heavy neutrino mass scale in the seesaw mechanism from experimental data on oscillations of solar and atmospheric neutrinos and quark-lepton symmetry. The resulting scale is around or…

High Energy Physics - Phenomenology · Physics 2009-10-31 D. Falcone

We have investigated a neutrino mass matrix model without supersymmetry including three see-saw right-handed neutrinos around order $10^{12}$ GeV masses, aiming at a picture with all small numbers explained as being due to approximately…

High Energy Physics - Phenomenology · Physics 2014-11-17 H. B. Nielsen , Y. Takanishi