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In this letter, we propose an extension of the scotogenic model where singlet Majorana particle can be dark matter (DM) without the need of a highly suppressed scalar coupling of the order $O(10^{-10})$. For that, the SM is extended with…

High Energy Physics - Phenomenology · Physics 2021-01-28 Amine Ahriche , Adil Jueid , Salah Nasri

The scotogenic model generates Majorana neutrino masses radiatively, with dark matter particles running in the loop. We explore the parameter space in which the relic density of fermionic dark matter is generated via a conversion-driven…

High Energy Physics - Phenomenology · Physics 2023-02-02 Julian Heeck , Jan Heisig , Anil Thapa

Modular symmetries have been impeccable in neutrino and quark sectors. This motivated us, therefore, to propose a variant of scotogenic model based on modular $A_4$ symmetry to realize the neutrino mass generation at one-loop level through…

High Energy Physics - Phenomenology · Physics 2020-09-04 Mitesh Kumar Behera , Shivaramakrishna Singirala , Subhasmita Mishra , Rukmani Mohanta

We propose a hybrid scotogenic inverse seesaw framework in which the Majorana mass term is generated at the one-loop level through the inclusion of a singlet fermion. This singlet Majorana fermion also serves as a viable thermal relic dark…

High Energy Physics - Phenomenology · Physics 2025-05-23 Gourab Pathak , Pritam Das , Mrinal Kumar Das

The singlet majoron model of seesaw neutrino mass is appended by one dark Majorana fermion singlet $\chi$ with $L=2$ and one dark complex scalar singlet $\zeta$ with $L=1$. This simple setup allows $\chi$ to obtain a small radiative mass…

High Energy Physics - Phenomenology · Physics 2021-09-15 Ernest Ma , Valentina De Romeri

We consider an extension of the standard model (SM) with an inert Higgs doublet and three Majorana singlet fermions to address both origin and the smallness of neutrino masses and dark matter (DM) problems. In this setup, the lightest…

High Energy Physics - Phenomenology · Physics 2018-05-22 Amine Ahriche , Adil Jueid , Salah Nasri

Non-zero neutrino mass and dark matter cast a shadow over the success of the Standard Model (SM) of Particle Physics. The most straightforward extension of the SM to explain these two phenomena is the Scotogenic model, where the SM particle…

High Energy Physics - Phenomenology · Physics 2023-02-08 Avnish , Kirtiman Ghosh

In this literature we show how the scotogenic frame work can be a common origin for explaining neutrino mass, lepton asymmetry and give a dark matter candidate. We start out with the extension of the Standard Model with fermions, which are…

High Energy Physics - Phenomenology · Physics 2023-03-08 Sumit Satapathy

In 2006, a simple extension of the Standard Model was proposed in which neutrinos obtain radiative Majorana masses at one-loop level from their couplings with dark matter, hence the term "scotogenic," from the Greek "scotos" meaning…

High Energy Physics - Phenomenology · Physics 2013-05-30 Yasaman Farzan , Ernest Ma

We propose that neutrino masses are "seeded" by a dark sector within the inverse seesaw mechanism. This way we have a new, "hidden", variant of the scotogenic scenario for radiative neutrino masses. We discuss both explicit and dynamical…

High Energy Physics - Phenomenology · Physics 2021-09-08 Sanjoy Mandal , Nicolás Rojas , Rahul Srivastava , José W. F. Valle

We review theoretical frameworks in which small neutrino masses arise radiatively through interactions with a dark sector that also accounts for cosmological dark matter (DM). A prototype is provided by scotogenic schemes, that extend the…

High Energy Physics - Phenomenology · Physics 2026-03-03 Ivania M. Ávila , Anirban Karan , Sanjoy Mandal , Soumya Sadhukhan , José W. F. Valle

A variation of the original 2006 radiative seesaw model of neutrino mass through dark matter is shown to realize the notion of inverse seesaw naturally. The dark-matter candidate here is the lightest of three real singlet scalars which may…

High Energy Physics - Phenomenology · Physics 2015-06-22 Sean Fraser , Ernest Ma , Oleg Popov

The scotogenic model of radiative neutrino mass with $Z_2$ or $U(1)_D$ dark matter is shown to accommodate $\Delta(27)$ symmetry naturally. The resulting neutrino mass matrix is identical to either of two forms, one proposed in 2006, the…

High Energy Physics - Phenomenology · Physics 2014-06-24 Ernest Ma , Alexander Natale

The unifiable supersymmetric left-right model where the neutral fermion $n$ in the $SU(2)_R$ doublet $(n,e)_R$ is a dark-matter candidate, is shown to have the requisite particle content for the neutrino $\nu$ in the $SU(2)_L$ doublet…

High Energy Physics - Phenomenology · Physics 2015-06-16 Subhaditya Bhattacharya , Ernest Ma , Daniel Wegman

In the framework of seesaw neutrino masses from heavy fermion triplets $(\Sigma^+,\Sigma^0,\Sigma^-)$, the addition of a light fermion singlet $N$ and a heavy scalar triplet $(\rho^+,\rho^0,\rho^-)$ has some important consequences. The new…

High Energy Physics - Phenomenology · Physics 2022-07-27 Ernest Ma

A minimal extension of the Standard Model is proposed, where the observed left-handed neutrinos obtain naturally small Majorana masses from a one-loop radiative seesaw mechanism. This model has two candidates (one bosonic and one fermionic)…

High Energy Physics - Phenomenology · Physics 2010-04-06 Ernest Ma

Assuming that neutrinos acquire radiative seesaw Majorana masses through their interactions with dark matter, i.e. scotogenic from the Greek 'scotos' meaning darkness, and using the non-Abelian discrete symmetry $A_4$, we propose a model of…

High Energy Physics - Phenomenology · Physics 2012-08-28 Ernest Ma , Alexander Natale , Ahmed Rashed

The seesaw mechanism with three heavy Majorana right-handed neutrinos provides an elegant explanation for neutrino masses and, combined with leptogenesis, can generate the baryon asymmetry of the universe (BAU). Naturally embedded in a…

High Energy Physics - Phenomenology · Physics 2025-05-06 Juan Herrero-Garcia , Giacomo Landini , Tsutomu T. Yanagida

We propose an economical model in which the tiny active neutrino masses arise from an interplay of linear and inverse seesaw mechanisms. The Standard Model is extended by a local $U(1)'$ gauge symmetry and discrete…

High Energy Physics - Phenomenology · Physics 2025-12-16 Asmaa Abada , Antonio Enrique Cárcamo Hernández , Salvador Urrea

Using a mechanism which allows naturally small Dirac neutrino masses and its linkage to a dark gauge $U(1)_D$ symmetry, a realistic Dirac neutrino mass matrix is derived from $S_3$. The dark sector naturally contains a fermion singlet…

High Energy Physics - Phenomenology · Physics 2021-03-17 Ernest Ma
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