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Observation of the neutrinoless double beta decay ($\0n$) has established that there is lepton number violation in nature and the neutrino masses are Majorana in nature. It also gives the absolute mass of the neutrinos and discriminates…

High Energy Physics - Phenomenology · Physics 2014-11-17 H. V. Klapdor-Kleingrothaus , U. Sarkar

Neutrinoless double beta decay is the only realistic probe of the Majorana nature of the neutrino. In the standard picture, its rate is proportional to $m_{ee}$, the e-e element of the Majorana neutrino mass matrix in the flavor basis. I…

High Energy Physics - Phenomenology · Physics 2009-06-30 James Jenkins

The small neutrino mass observed in neutrino oscillations is nicely explained by the seesaw mechanism. Rich phenomenology is generally expected if the heavy neutrinos are not much heavier than the electroweak scale. A model with this…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jian-Ping Bu , Yi Liao , Ji-Yuan Liu

Leptogenesis in a left-right symmetric model is investigated for all possible neutrino mass hierarchies. The predictions of the model for low energy parameters as measured in neutrinoless double beta decay and in oscillation experiments are…

High Energy Physics - Phenomenology · Physics 2010-04-05 Werner Rodejohann

We study the range of the elements of the neutrino mass matrix m_nu in the charged lepton basis. Neutrino-less double beta decay is sensitive to the ee element of m_nu. We then analyze the phenomenological implications of single texture…

High Energy Physics - Phenomenology · Physics 2011-06-24 A. Merle , W. Rodejohann

The current neutrino experiments provide an opportunity for testing the inverse see-saw mechanism through charged lepton flavor violating processes and neutrinoless double beta decay. Motivated by this, in this paper we study the…

High Energy Physics - Phenomenology · Physics 2024-11-07 Juan Carlos Gómez-Izquierdo , Catalina Espinoza , Lucia E. Gutiérrez Luna , Myriam Mondragón

We discuss a mechanism of neutrinoless double beta decay, where neutrinos of different flavours come into play. This is realized by effective flavour-violating scalar interactions. As one consequence, we find that within the normal mass…

High Energy Physics - Phenomenology · Physics 2021-03-15 Lukas Graf , Sudip Jana , Manfred Lindner , Werner Rodejohann , Xun-Jie Xu

We study the new physics contributions to neutrinoless double beta decay ($0\nu\beta \beta$) half-life and lepton flavour violation (LFV) amplitude within the framework of the minimal left-right symmetric model (MLRSM). Considering all…

High Energy Physics - Phenomenology · Physics 2016-08-03 Debasish Borah , Arnab Dasgupta

The discovery of neutrino masses has raised the importance of studies in the context of neutrinoless double beta decay, which constitutes a landmark for lepton number violation. The standard interpretation is that the light massive…

High Energy Physics - Phenomenology · Physics 2018-05-25 A. C. O. Santos , P. Vasconcelos

A mechanism has been suggested recently to generate the neutrino mass out of a dimension-seven operator. This is expected to relieve the tension between the occurrence of a tiny neutrino mass and the observability of other physics effects…

High Energy Physics - Phenomenology · Physics 2010-12-24 Yi Liao , Guo-Zhu Ning , Lu Ren

Lepton-number violation (LNV), in general, implies nonzero Majorana masses for the Standard Model neutrinos. Since neutrino masses are very small, for generic candidate models of the physics responsible for LNV, the rates for almost all…

High Energy Physics - Phenomenology · Physics 2019-10-30 André de Gouvêa , Wei-Chih Huang , Johannes König , Manibrata Sen

Neutrinoless double beta decay is the most powerful tool to probe not only for Majorana neutrino masses but for lepton number violating physics in general. We discuss relations between lepton number violation, double beta decay and neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-11 Frank F. Deppisch , Martin Hirsch , Heinrich Päs

We revisit the thermal leptogenesis scenario in the type-I seesaw framework featuring three heavy Majorana neutrinos with a hierarchical mass spectrum. We focus on low energy observables, specifically the lightest neutrino mass…

High Energy Physics - Phenomenology · Physics 2025-07-21 Alessandro Granelli , Koichi Hamaguchi , Maura E. Ramirez-Quezada , Kengo Shimada , Juntaro Wada , Tatsuya Yokoyama

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 analyze neutrino masses and Lepton Flavor Violation (LFV) in charged leptons with a minimal ansatz about the breaking of the U(3)^5 flavor symmetry, consistent with the U(2)^3 breaking pattern of quark Yukawa couplings, in the context of…

High Energy Physics - Phenomenology · Physics 2015-06-04 Gianluca Blankenburg , Gino Isidori , Joel Jones-Perez

The predictions for the effective Majorana mass |<m>| in neutrinoless double-beta decay in the case of 3-neutrino mixing and massive Majorana neutrinos are reviewed. The physics potential of the experiments, searching for neutrinoless…

High Energy Physics - Phenomenology · Physics 2007-05-23 S. Pascoli , S. T. Petcov

In the light of KamLAND data just released, we reanalyze and update the constraints on neutrino masses and mixing parameters, the most general ones that can be derived in three-flavor mixing scheme of neutrinos with use of the bounds…

High Energy Physics - Phenomenology · Physics 2014-11-17 Hisakazu Minakata , Hiroaki Sugiyama

In the context of left-right symmetric models we study the connection of leptogenesis and low energy parameters such as neutrinoless double beta decay and leptonic CP violation. Upon imposition of a unitarity constraint, the neutrino…

High Energy Physics - Phenomenology · Physics 2009-11-07 K. R. S. Balaji , W. Rodejohann

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

The effective Majorana mass which determines the rate of the neutrinoless double beta decay, |<m>|, is considered in the case of three-neutrino mixing and massive Majorana neutrinos. Assuming a rather precise determination of the parameters…

High Energy Physics - Phenomenology · Physics 2011-04-20 S. Pascoli , S. T. Petcov , L. Wolfenstein