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Related papers: Three-loop Neutrino Mass Model with Doubly Charged…

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In this work, we report on recent analysis of three-loop models of neutrino mass with dark matter. We discuss in detail the model of Krauss-Nasri-Trodden (KNT) [1], showing that it offers a viable solution to the neutrino mass and dark…

High Energy Physics - Phenomenology · Physics 2015-04-28 Amine Ahriche , Kristian L. McDonald , Salah Nasri

In the simplest scheme for neutrino masses invoking a triplet of Higgs scalars there are two CP-even neutral Higgs bosons $H_i$ (i=1,2) and one massive pseudoscalar $A$. For some choices of parameters, the lightest $H_1$ may be lighter than…

High Energy Physics - Phenomenology · Physics 2009-09-17 M. A. Diaz , M. A. Garcia-Jareno , D. A. Restrepo , J. W. F. Valle

We propose a low scale leptogenesis scenario in the framework of composite Higgs models supplemented with singlet heavy neutrinos. One of the neutrinos can also be considered as a dark matter candidate whose stability is guaranteed by a…

High Energy Physics - Phenomenology · Physics 2021-04-28 M. Ahmadvand

We consider the extension of the Standard Model with an inert scalar doublet, three right-handed neutrinos, and singlet scalar fields, $\varphi$ and $S$. In this model, neutrino masses are zero in the limit of the unbroken $Z_4$ discrete…

High Energy Physics - Phenomenology · Physics 2025-07-18 Jongkuk Kim , Seong-Sik Kim , Hyun Min Lee , Rojalin Padhan

Neutrino are massless in the Standard Model. The most popular mechanism to generate neutrino masses are the type I and type II seesaw, where right-handed neutrinos and a scalar triplet are augmented to the Standard Model, respectively. In…

High Energy Physics - Phenomenology · Physics 2020-01-08 Manoel M. Ferreira , Tessio B. de Melo , Sergey Kovalenko , Paulo R. D. Pinheiro , Farinaldo S. Queiroz

The inability to predict neutrino masses and the existence of the dark matter are two essential shortcomings of the Standard Model. The Higgs Triplet Model provides an elegant resolution of neutrino masses via the seesaw mechanism. We show…

High Energy Physics - Phenomenology · Physics 2015-09-16 Sahar Bahrami , Mariana Frank

We present a model of radiative neutrino masses which also resolves anomalies reported in $B$-meson decays, $R_{D^{(\star)}}$ and $R_{K^{(\star)}}$, as well as in muon $g-2$ measurement, $\Delta a_\mu$. Neutrino masses arise in the model…

High Energy Physics - Phenomenology · Physics 2021-03-31 K. S. Babu , P. S. Bhupal Dev , Sudip Jana , Anil Thapa

We propose a one-loop induced radiative neutrino mass model with anomaly free flavour dependent gauge symmetry: $\mu$ minus $\tau$ symmetry $U(1)_{\mu-\tau}$. A neutrino mass matrix satisfying current experimental data can be obtained by…

High Energy Physics - Phenomenology · Physics 2015-06-23 Seungwon Baek , Hiroshi Okada , Kei Yagyu

Babu studied the neutrino spectrum obtained when one adds a charged singlet and a doubly charged singlet to the standard model particle spectrum. It was found that the neutrinos acquire a mass matrix at the two-loop level which contains one…

High Energy Physics - Phenomenology · Physics 2007-05-23 K. L. McDonald , B. H. J. McKellar

Motivated by the interesting features of Two Higgs Doublet Models (2HDM) we present a 2HDM extension where the stability of dark matter, neutrino masses and the absence of flavor changing interactions are explained by promoting baryon and…

High Energy Physics - Phenomenology · Physics 2019-06-19 Daniel A. Camargo , Miguel D. Campos , Téssio B. de Melo , Farinaldo S. Queiroz

The latest results of CDF-II collaboration show a discrepancy of $7\sigma$ with standard model expectations. There is, also, a $4.2\sigma$ discrepancy in the measurement of muon magnetic moment reported by Fermilab. We study the connection…

High Energy Physics - Phenomenology · Physics 2022-07-19 Simran Arora , Monal Kashav , Surender Verma , B. C. Chauhan

Small neutrino masses can be sourced by a tiny vacuum expectation value of a leptophilic Higgs doublet, and mediated by Quasi-Dirac heavy neutrinos. In such simplest linear seesaw picture the neutrino mass mediators can be accessible to…

High Energy Physics - Phenomenology · Physics 2025-01-03 Aditya Batra , Praveen Bharadwaj , Sanjoy Mandal , Rahul Srivastava , José W. F. Valle

We propose a neutrino model in which neutrino masses are generated at one loop level and three right-handed fermions have non-trivial charges under $U(1)_{B-L}$ gauge symmetry in no conflict with anomaly cancellation. After the…

High Energy Physics - Phenomenology · Physics 2019-03-06 Takaaki Nomura , Hiroshi Okada

We propose a class of models providing an explanation of the origin of light neutrino masses, the baryon asymmetry of the Universe via leptogenesis and offering viable dark matter candidates. In these models the Majorana masses of the…

High Energy Physics - Phenomenology · Physics 2024-04-11 Asmaa Abada , Nicolás Bernal , Antonio E. Cárcamo Hernández , Sergey Kovalenko , Téssio B. de Melo

In this work, we interpret the 3-3-1-1 model when the B-L and 3-3-1 breaking scales behave simultaneously as the inflation scale. This setup not only realizes the previously-achieved consequences of inflation and leptogenesis, but also…

High Energy Physics - Phenomenology · Physics 2017-04-04 D. T. Huong , P. V. Dong

I present several scenarios developed in Zagreb, in which TeV-scale particles belonging to non-trivial weak-isospin multiplets give rise to neutrino-mass mechanisms different from conventional type I, II and III seesaw models. Two dim 9…

High Energy Physics - Phenomenology · Physics 2019-03-29 Ivica Picek

The type II seesaw mechanism introduces a hypercharged Higgs triplet to explain the observed neutrino masses and mixing. Among three triplet components, the doubly charged Higgs boson can be the lightest and decay mainly to same-sign…

High Energy Physics - Phenomenology · Physics 2012-09-07 Eung Jin Chun , Pankaj Sharma

We propose a model based on the gauge group $SU(3)_{C}\otimes SU(3)_{L}\otimes U(1)_{X}$ with an extra $S_{3}$ flavor symmetry, which accounts for the lepton masses and mixing. The small active neutrino masses are generated via a double…

High Energy Physics - Phenomenology · Physics 2014-10-15 A. E. Cárcamo Hernández , E. Cataño Mur , R. Martinez

We study neutrino mass generation and dark matter in a left-right symmetric model. The model is based on an $SU(3)_c\times SU(2)_L \times SU(2)_R \times U(1)_{B-L}$ gauge theory with a softly broken parity symmetry. Masses of the charged…

High Energy Physics - Phenomenology · Physics 2025-10-07 Shohei Okawa , Yuji Omura , Keyun Wu

Motivated by searches for so-called leptonic scalars at the LHC and the recent measurement of the $W$ boson's mass at the Tevatron, we revisit the phenomenology of the Zee-Babu model for neutrino masses and the ability to differentiate it…

High Energy Physics - Phenomenology · Physics 2022-11-03 Richard Ruiz
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