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Related papers: Littlest Inverse Seesaw Model

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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 introduce three right-handed neutrinos and three sterile neutrinos, and consider an inverse seesaw mechanism for neutrino mass generation. From naturalness point of view, their Majorana masses should be small, while it induces a large…

High Energy Physics - Phenomenology · Physics 2016-11-10 Naoyuki Haba , Hiroyuki Ishida , Yuya Yamaguchi

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

We investigate models of charged lepton and neutrino masses and lepton mixing based on broken modular symmetry. The matter fields in these models are assumed to transform in irreducible representations of the finite modular group $\Gamma_4…

High Energy Physics - Phenomenology · Physics 2019-05-01 P. P. Novichkov , J. T. Penedo , S. T. Petcov , A. V. Titov

We studied models of leptogenesis where three right-handed Majorana neutrinos are involved and the minimal-extended seesaw mechanism including an additional singlet field produces four light neutrinos. This study shows that the type of mass…

High Energy Physics - Phenomenology · Physics 2022-12-28 Ki-Young Jung , Kim Siyeon

We suggest a simple model, based on the type-I seesaw mechanism, for the lepton mass matrices. The model hinges on an Abelian symmetry which leads to mass matrices with some vanishing matrix elements. The model predicts one massless…

High Energy Physics - Phenomenology · Physics 2015-06-04 P. M. Ferreira , L. Lavoura

The seesaw model of heavy and light Majorana neutrinos and its low-energy effective theory are studied, when the number of heavy neutrinos is equal to or less than the number of light lepton generations. We establish a general relationship…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. Broncano , M. B. Gavela , E. Jenkins

The advent of the LHC, and the proposal of building future colliders as the ILC, both programmed to explore new physics at the TeV scale, justifies the recent interest in studying all kind of seesaw mechanisms whose signature lies on such…

High Energy Physics - Phenomenology · Physics 2017-03-15 F. F. Freitas , C. A. de S. Pires , P. S. Rodrigues da Silva

We introduce a lepton mass generation and flavor mixing model, realized through a (2,3) inverse seesaw structure based on modular \( S_4 \) symmetry. The model employs modular forms to construct the lepton Yukawa couplings, significantly…

High Energy Physics - Phenomenology · Physics 2025-09-23 Abhishek , V. Suryanarayana Mummidi

We present a type-III version of inverse seesaw or, equivalently an inverse version of type-III seesaw. Naturally small neutrino masses arise at low-scale from the exchange of neutral fermions transforming as hyperchargeless SU(2) triplets.…

High Energy Physics - Phenomenology · Physics 2009-11-06 D. Ibanez , S. Morisi , J. W. F. Valle

We study the possibility of simultaneously addressing neutrino phenomenology and the dark matter in the framework of inverse seesaw. The model is the extension of the standard model by the addition of two right handed neutrinos and three…

High Energy Physics - Phenomenology · Physics 2020-02-19 Nayana Gautam , Mrinal Kumar Das

In many extensions of the Standard Model, including a broad class of left-right symmetric and Grand Unified theories, the light neutrino mass matrix is given by the left-right symmetric seesaw formula $M_\nu = f v_L - \frac{v^2}{v_R} Y_\nu…

High Energy Physics - Phenomenology · Physics 2009-11-11 Pierre Hosteins , Stephane Lavignac , Carlos A. Savoy

Current data implies three simple forms of the neutrino mass matrix, each corresponding to the conservation of a non-standard lepton charge. While models based on L_e and L_e - L_mu - L_tau are well-known, little attention has been paid to…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Rodejohann , M. A. Schmidt

In the context of Standard Model (SM) extensions, the seesaw mechanism provides the most natural explanation for the smallness of neutrino masses. In this work we consider the most economical type-I seesaw realization in which two…

High Energy Physics - Phenomenology · Physics 2018-06-20 D. M. Barreiros , R. G. Felipe , F. R. Joaquim

The explanation of the small neutrino mass can be depicted using some handsome models like type-I and inverse seesaw where the Standard Model gauge singlet heavy right handed neutrinos are deployed. The common thing in these two models is a…

High Energy Physics - Phenomenology · Physics 2021-03-04 Arindam Das

The simplest type III seesaw model as originally proposed introduces one lepton triplet. It thus contains four active neutrinos, two massive and two massless at tree level. We determine the radiative masses that the latter receive first at…

High Energy Physics - Phenomenology · Physics 2009-04-22 Yi Liao , Ji-Yuan Liu , Guo-Zhu Ning

We study lepton flavor violation (LFV) within the Littlest Higgs Model with T parity (LHT) realizing an inverse seesaw (ISS) mechanism of type I. With respect to the traditional LHT, there appear new $\mathcal{O}$(\textcolor{black}{10} TeV)…

High Energy Physics - Phenomenology · Physics 2022-02-10 Iván Pacheco , Pablo Roig

We consider supersymmetric models in which the right-handed sneutrino is a viable WIMP dark matter candidate. These are either simple extensions of the Minimal Supersymmetric Standard Model or models with the addition of an extra U(1)…

High Energy Physics - Phenomenology · Physics 2012-09-10 Valentina De Romeri

The type II seesaw mechanism is an attractive way to generate the observed light neutrino masses. It postulates a SU(2)$_\mathrm{L}$-triplet scalar field, which develops an induced vacuum expectation value after electroweak symmetry…

High Energy Physics - Phenomenology · Physics 2019-03-01 Stefan Antusch , Oliver Fischer , A. Hammad , Christiane Scherb

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