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Related papers: Radiative Two-Loop Neutrino Masses with Dark Matte…

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In the context of a left-right extension of the standard model of quarks and leptons with the addition of a gauged $U(1)_D$ dark symmetry, it is shown how the electron may obtain a radiative mass in one loop and two Dirac neutrinos obtain…

High Energy Physics - Phenomenology · Physics 2021-02-17 Ernest Ma

We investigate a radiative seesaw model with two leptoquarks under non-holomorphic modular $A_4$ symmetry. The leptons and quarks belong to non-trivial representations of the modular $A_4$ and the structures of their mass matrices are…

High Energy Physics - Phenomenology · Physics 2025-05-14 Takaaki Nomura , Hiroshi Okada , Xing-Yu Wang

Supersymmetric radiative neutrino mass models have often two dark matter candidates. One is the usual lightest neutralino with odd R parity and the other is a new neutral particle whose stability is guaranteed by a discrete symmetry that…

High Energy Physics - Phenomenology · Physics 2011-07-07 Hiroki Fukuoka , Daijiro Suematsu , Takashi Toma

We propose a Standard Model (SM) extension where neutrinos get masses through a two-loop inverse seesaw mechanism. This naturally explains the smallness of the neutrino masses and allows seesaw mediators to be at the TeV scale with testable…

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 compute one loop neutrino masses in the R-parity violating Minimal Supersymmetric Model, including the bilinear R-parity violating masses in the mass insertion approximation. To the order we calculate, our results are independent of the…

High Energy Physics - Phenomenology · Physics 2009-10-31 Sacha Davidson , Marta Losada

Within the framework of the complete theory of supersymmetry without R-parity, where all possible R-parity violating terms are admitted, we perform a systematic analytical study of all sources of neutrino masses up to ``direct one-loop"…

High Energy Physics - Phenomenology · Physics 2014-11-17 Otto C. W. Kong

In an attempt to unfold (if any) a possible connection between two apparently uncorrelated sectors, namely neutrino and dark matter, we consider the type-I seesaw and a fermion singlet dark matter to start with. Our construction suggests…

High Energy Physics - Phenomenology · Physics 2018-12-26 Subhaditya Bhattacharya , Ivo de Medeiros Varzielas , Biswajit Karmakar , Stephen F. King , Arunansu Sil

We study the generation of neutrino masses in the $SU(3)_W$ electroweak unified theory in $M_4\times S_1/(Z_2\times Z'_2)$ spacetime. By appropriate orbifolding, the bulk symmetry $SU(3)_W$ is broken into $SU(2)_L \times U(1)_Y$ at one of…

High Energy Physics - Phenomenology · Physics 2011-07-19 Chia-Hung V. Chang , We-Fu Chang , John N. Ng

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

We propose a two-loop induced Zee-Babu type neutrino mass model at the TeV scale. Although there is no dark matter candidate in the original Zee-Babu model, that is contained in our model by introducing an unbroken discrete $Z_2$ symmetry.…

High Energy Physics - Phenomenology · Physics 2014-11-11 Hiroshi Okada , Takashi Toma , Kei Yagyu

The well-studied radiative model of neutrino mass through $Z_2$ dark matter is shown to be naturally realizable in the context of SU(6) grand unification. A recent new proposal based on U(1)_D dark matter is similarly accommodated in SU(7).…

High Energy Physics - Phenomenology · Physics 2015-06-16 Ernest Ma

We discuss the generation of small neutrino masses from effective operators higher than dimension five, which open new possibilities for low scale see-saw mechanisms. In order to forbid the radiative generation of neutrino mass by lower…

High Energy Physics - Phenomenology · Physics 2009-11-23 Florian Bonnet , Daniel Hernandez , Toshihiko Ota , Walter Winter

Despite direct observations favoring a low mass density, a critical density universe with a neutrino component of dark matter provides the best existing model to explain the observed structure of the universe over more than three orders of…

Astrophysics · Physics 2009-10-31 David O. Caldwell

We propose a predictively radiative neutrino mass model with gauged $U(1)_{B-2L_{\ell_2}-L_{\ell_1}}$ symmetry in which we successfully realize two-zero textures of neutrino mass matrix depending on charge assignment for leptons and the…

High Energy Physics - Phenomenology · Physics 2018-06-27 Takaaki Nomura , Hiroshi Okada

We present a renormalizable flavor model with Z_4 as flavor symmetry in both the quark and lepton sectors. The model is constructed with a minimal approach and no-right handed neutrinos are introduced. In this approach a minimum number of…

High Energy Physics - Phenomenology · Physics 2013-05-30 Alfredo Aranda , Cesar Bonilla , Alma D. Rojas

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

We discuss the connection between the origin of neutrino masses and their mixings which arises in a class of scenarios with radiatively induced neutrino masses. In these scenarios, the neutrino mass matrix acquires textures with two entries…

High Energy Physics - Phenomenology · Physics 2014-07-18 Michael Gustafsson , Jose M. No , Maximiliano A. Rivera

An anomaly-free U(1) gauge extension of the standard model (SM) is presented. Only one Higgs doublet with a nonzero vacuum expectation is required as in the SM. New fermions and scalars as well as all SM particles transform nontrivially…

High Energy Physics - Phenomenology · Physics 2016-02-23 Rathin Adhikari , Debasish Borah , Ernest Ma

There exist several distinct phenomenological models to generate neutrino masses. We explore, which of these models can consistently be embedded in a quantum theory of gravity and matter. We proceed by invoking a minimal number of degrees…

High Energy Physics - Phenomenology · Physics 2025-05-05 Gustavo P. de Brito , Astrid Eichhorn , Antonio D. Pereira , Masatoshi Yamada
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