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Related papers: Minimal Dark Matter and Leptogenesis

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The minimal seesaw extension of the Standard SU(3) x SU(2) x U(1) Model requires two electroweak singlet fermions in order to accommodate the neutrino oscillation parameters at tree level. Here we consider a next to minimal extension where…

High Energy Physics - Phenomenology · Physics 2013-11-05 M. Hirsch , R. A. Lineros , S. Morisi , J. Palacio , N. Rojas , J. W. F. Valle

Associated with two TeV-scale leptoquark scalars, a dark matter fermion which is the neutral component of an isotriplet can mediate a testable neutrinoless double beta decay at one-loop level. The dark matter fermion with determined mass…

High Energy Physics - Phenomenology · Physics 2012-09-14 Pei-Hong Gu

We study Majoron dark matter (DM) in its minimal realization, based on the Type-I seesaw framework extended by a SM-singlet complex scalar. Remaining agnostic about the origin and value of the Majoron mass, we evaluate the DM abundance from…

High Energy Physics - Phenomenology · Physics 2026-05-14 Kensuke Akita , Koichi Hamaguchi , Haruto Kitagawa , Tatsuya Yokoyama

We formulate a predictive model of fermion masses and mixings based on a $\Delta(27)$ family symmetry. In the quark sector the model leads to the viable mixing inspired texture where the Cabibbo angle comes from the down quark sector and…

High Energy Physics - Phenomenology · Physics 2018-06-13 Nicolás Bernal , A. E. Cárcamo Hernández , Ivo de Medeiros Varzielas , Sergey Kovalenko

In this paper we work in the framework of a radiative seesaw model with triplet fermion $\Sigma$. Due to the $Z_2$ discrete flavor symmetry, the lightest neutral component of $\Sigma$ is stable and thus can be a dark matter candidate. Its…

High Energy Physics - Phenomenology · Physics 2012-03-01 Wei Chao

We study leptogenesis in three different realisations of the type Ib seesaw mechanism, where the effective masses of the neutrinos are obtained by the spontaneous symmetry breaking of two different Higgs doublets. In the minimal type Ib…

High Energy Physics - Phenomenology · Physics 2022-04-05 Bowen Fu , Stephen F. King

The type III seesaw mechanism for neutrino mass generation usually makes use of at least two $Y = 0$, $SU(2)_L$ lepton triplets. We augment such a model with a third triplet and a sterile neutrino, both of which are odd under a conserved…

High Energy Physics - Phenomenology · Physics 2015-04-01 Avinanda Chaudhuri , Najimuddin Khan , Biswarup Mukhopadhyaya , Subhendu Rakshit

Asymmetric dark matter (ADM) has been an attractive possibility attempting to explain the observed ratio of baryon to dark matter abundance in the universe. While a bosonic ADM is constrained by the limits from existence of old neutron…

High Energy Physics - Phenomenology · Physics 2013-10-08 Biplob Bhattacherjee , Shigeki Matsumoto , Satyanarayan Mukhopadhyay , Mihoko M. Nojiri

A ~5 GeV `dark baryon' with a cosmic asymmetry similar to that of baryons is a natural candidate for the dark matter. We study the possibility of generating such a state through dynamical electroweak symmetry breaking, and show that it can…

High Energy Physics - Phenomenology · Physics 2011-09-28 Mads T. Frandsen , Subir Sarkar , Kai Schmidt-Hoberg

Neutrino masses could originate in seesaw models testable at colliders, with light mediators and an approximate lepton number symmetry. The minimal model of this type contains two quasi-degenerate Majorana fermions forming a pseudo-Dirac…

High Energy Physics - Phenomenology · Physics 2019-03-27 P. Hernández , J. Jones-Pérez , O. Suarez-Navarro

We explore a novel possibility that dark matter has a light mass below 1GeV in a lepton portal dark matter model. There are Yukawa couplings involving dark matter, left-handed leptons and an extra scalar doublet in the model. In the light…

High Energy Physics - Phenomenology · Physics 2022-09-13 Shohei Okawa , Yuji Omura

We consider an SU(3)'_c\times SU(2)'_L\times U(1)'_Y mirror sector where the field content and dimensionless couplings are a copy of the SU(3)_c\times SU(2)_L\times U(1)_Y ordinary sector. Our model also contains three gauge-singlet…

High Energy Physics - Phenomenology · Physics 2015-06-15 Pei-Hong Gu

Neutrinos may be Dirac particles whose masses arise radiatively at one-loop, naturally explaining their small values. In this work we show that all the one-loop realizations of the dimension-five operator to effectively generate Dirac…

High Energy Physics - Phenomenology · Physics 2019-05-17 Julian Calle , Diego Restrepo , Carlos E. Yaguna , Óscar Zapata

We demonstrate a common origin for high-scale leptogenesis and three-loop neutrino mass generation. Specifically we extend the standard model by two real singlet scalars, two singly charged scalars carrying different lepton numbers and two…

High Energy Physics - Phenomenology · Physics 2017-05-24 Pei-Hong Gu

The Dirac Scotogenic model provides an elegant mechanism for generating small Dirac neutrino masses at the one-loop level. A single abelian discrete $Z_{6}$ symmetry simultaneously protects the ``Diracness'' of the neutrinos and the…

High Energy Physics - Phenomenology · Physics 2025-04-16 Salvador Centelles Chuliá , Rahul Srivastava , Sushant Yadav

The extension of the Standard model (SM) with three heavy right handed neutrinos, a complex scalar and the gauged $U(1)_{\rm B-L}$ symmetry (the minimal $B-L$ model) is considered the most compelling minimal one: the presence and the…

High Energy Physics - Phenomenology · Physics 2021-01-19 Gongjun Choi , Tsutomu T. Yanagida , Norimi Yokozaki

We show that the mass of a self-interacting dark matter candidate, specifically a Dirac fermion, can be generated by composite dynamics, with a light scalar mediator emerging alongside the Higgs itself as composite particles. These novel…

High Energy Physics - Phenomenology · Physics 2024-12-30 Martin Rosenlyst

We propose an appealing alternative scenario of leptogenesis assisted by dark sector which leads to the baryon asymmetry of the Universe satisfying all theoretical and experimental constraints. The dark sector carries a non minimal set up…

High Energy Physics - Phenomenology · Physics 2021-03-05 Partha Konar , Ananya Mukherjee , Abhijit Kumar Saha , Sudipta Show

It is often said that asymmetric dark matter is light compared to typical weakly interacting massive particles. Here we point out a simple scheme with a neutrino portal and $\mathcal{O}(60 \text{ GeV})$ asymmetric dark matter which may be…

High Energy Physics - Phenomenology · Physics 2022-10-19 Eleanor Hall , Robert McGehee , Hitoshi Murayama , Bethany Suter

In the present universe visible and dark matter contribute comparable energy density although they have different properties. This coincidence can be elegantly explained if the dark matter relic density, originating from a dark matter…

High Energy Physics - Phenomenology · Physics 2011-09-05 Pei-Hong Gu , Manfred Lindner , Utpal Sarkar , Xinmin Zhang