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Weakly Interacting Massive Particles (WIMPs) and axions are arguably the most compelling dark matter (DM) candidates in the literature. Here, we consider a model where the PQ symmetry solves the strong CP problem, generates radiatively…

High Energy Physics - Phenomenology · Physics 2024-07-30 Robinson Longas , Andres Rivera , Cristian Ruiz , David Suarez

We study a minimal one-loop radiative mechanism for generating small Majorana neutrino masses in inverse seesaw extensions of the Standard Model with two singlet fermions per family. The new feature of this radiative mechanism is that the…

High Energy Physics - Phenomenology · Physics 2013-05-30 P. S. Bhupal Dev , Apostolos Pilaftsis

We propose that all light fermionic degrees of freedom, including the Standard Model (SM) fermions and all possible light beyond-the-standard-model fields, are chiral with respect to some spontaneously broken abelian gauge symmetry.…

High Energy Physics - Phenomenology · Physics 2015-07-06 André de Gouvea , Daniel Hernandez

Motivated by the recently reported excess in electron recoil events by the XENON1T collaboration, we propose an inelastic fermion dark matter (DM) scenario within the framework of a gauged $L_{\mu}-L_{\tau}$ extension of the standard model…

High Energy Physics - Phenomenology · Physics 2020-12-30 Debasish Borah , Satyabrata Mahapatra , Dibyendu Nanda , Narendra Sahu

We construct two viable extensions of the SM with a heavy vector in the fundamental $SU\left( 2\right) _{L}$ representation and nine SM singlet scalar fields, consistent with the current SM fermion mass spectrum and fermionic mixing…

High Energy Physics - Phenomenology · Physics 2019-09-24 A. E. Cárcamo Hernández , Jonatan Vignatti , Alfonso Zerwekh

The sfermion-mass spectrum of the minimal supersymmetric standard model is investigated at the one-loop level. An on-shell scheme has been specified for renormalization of the basic breaking parameters of the sfermionic sector. Owing to…

High Energy Physics - Phenomenology · Physics 2009-11-10 W. Hollik , H. Rzehak

In this paper we propose a radiated linear seesaw model where the naturally small term $\mu_{L}$ are generated at one-loop level and its soft-breaking of lepton number symmetry attributes to the spontaneous breaking(SSB) of B-L gauge…

High Energy Physics - Phenomenology · Physics 2015-11-05 Weijian Wang , Zhi-Long Han

We propose a left-right symmetric electroweak extension of the Standard Model based on the $\Delta \left( 27\right)$ family symmetry. The masses of all electrically charged Standard Model fermions lighter than the top quark are induced by a…

High Energy Physics - Phenomenology · Physics 2019-05-14 A. E. Cárcamo Hernández , Sergey Kovalenko , José W. F. Valle , C. A. Vaquera-Araujo

We discuss a one loop model for neutrino masses which leads to a seesaw-like formula with the difference that the charged lepton masses replace the unknown Dirac mass matrix present in the usual seesaw case. This is a considerable reduction…

High Energy Physics - Phenomenology · Physics 2009-12-10 Adisorn Adulpravitchai , Manfred Lindner , Alexander Merle , Rabindra N. Mohapatra

We point out that the minimal seesaw model can provide a natural framework to accommodate tiny neutrino masses, while its experimental testability and notable predictiveness are still maintained. This possibility is based on the observation…

High Energy Physics - Phenomenology · Physics 2010-05-12 He Zhang , Shun Zhou

We propose an inverse seesaw model with large $SU(2)_L$ multiplet fields which realizes natural mass hierarchies among neutral fermions. Here, lighter neutral fermion mass matrices are induced via two suppression mechanisms; one is small…

High Energy Physics - Phenomenology · Physics 2019-04-10 Takaaki Nomura , Hiroshi Okada

We discuss a mechanism where charged lepton masses are derived from one-loop diagrams mediated by particles in a dark sector including a dark matter candidate. We focus on a scenario where the muon and electron masses are generated at one…

High Energy Physics - Phenomenology · Physics 2021-09-08 Cheng-Wei Chiang , Kei Yagyu

If neutrinos have masses, why are they so tiny? Are these masses of the Dirac type or of the Majorana type? We are already familiar with the mechanism of how to obtain a tiny Majorana neutrino mass by the famous see-saw mechanism. The…

High Energy Physics - Phenomenology · Physics 2009-10-31 P. Q. Hung

A new dynamical symmetry breaking model of electroweak interactions is proposed based on interacting fermions. Two fermions of different SU_{L}(2) representations form a symmetry breaking condensate and generate the lepton and quark masses.…

High Energy Physics - Phenomenology · Physics 2009-01-07 G. Cynolter , E. Lendvai , G. Pocsik

We propose a "scotogenic" mechanism relating small neutrino mass and cosmological dark matter. Neutrinos are Dirac fermions with masses arising only in two--loop order through the sector responsible for dark matter. Two triality symmetries…

High Energy Physics - Phenomenology · Physics 2016-09-21 Cesar Bonilla , Ernest Ma , Eduardo Peinado , Jose W. F. Valle

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

We demonstrate that an $SU(2)_L\times U(1)_Y$ model with the same particle content as Standard Model(SM) and discrete reflection symmetry between second and third generation of leptons give rise to charged lepton and neutrino mass matrices…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ambar Ghosal

We construct a simple model of fermion masses based on a spontaneously broken S3 X Z3 flavour group. At the leading order, in the neutrino sector S3 is broken down to a \nu_\mu-\nu_\tau parity subgroup that enforces a maximal atmospheric…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ferruccio Feruglio , Yin Lin

The gauge symmetry of the Standard Model is SU(3)_c x SU(2)_L x U(1)_Y for unknown reasons. One aspect that can be addressed is the low dimensionality of all its subgroups. Why not much larger groups like SU(7), or for that matter, SP(38)…

High Energy Physics - Phenomenology · Physics 2016-12-30 Guillermo Garcia Fernandez , Jesus Guerrero Rojas , Felipe J. Llanes-Estrada

We show that composite fermions with masses much smaller than the scale of confinement arise naturally in certain models which admit dynamical breakdown of chiral symmetry. The models are such that to leading order some of the fermions…

High Energy Physics - Phenomenology · Physics 2016-09-01 Pankaj Jain