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Using the Weinberg operator, we present a full collection of genuine two-loop models for neutrino mass generation, which contain a dark matter particle as one of the internal messengers. These models can be constructed simply by adding new…

High Energy Physics - Phenomenology · Physics 2017-05-24 C. Simoes , D. Wegman

The beyond-the-standard-model scenario in this work is motivated from the observations of neutrino masses, anomalous magnetic moments of electron and muon, and dark matter in the Universe. We explain these observations by extending the…

High Energy Physics - Phenomenology · Physics 2026-05-11 Vandana Sahdev

The properties of light leptoquarks predicted in the context of a simple grand unified theory and their observability at the LHC are investigated. The SU(5) symmetry of the theory implies that the leptoquark couplings to matter are related…

High Energy Physics - Phenomenology · Physics 2009-05-28 Pavel Fileviez Perez , Tao Han , Tong Li , Michael J. Ramsey-Musolf

We consider the radiative generation of neutrino mass through the interactions of neutrinos with MeV dark matter. We construct a realistic renormalizable model with one scalar doublet and one complex singlet together with three light…

High Energy Physics - Phenomenology · Physics 2016-07-15 Abdesslam Arhrib , Céline Bœhm , Ernest Ma , Tzu-Chiang Yuan

In this work we study examples of hierarchical neutrino mass matrices inspired by family symmetries, compatible with experiments on neutrino oscillations, and for which there is a connection among the low energy CP violation phase…

High Energy Physics - Phenomenology · Physics 2009-11-10 L. Velasco-Sevilla

We propose a model based on the gauge group $SU(4)\times SU(2)_L\times SU(2)_R$ where the Dirac masses of all the known fermions are generated as one-loop radiative corrections. We are able to generate realistic quark and lepton masses and…

High Energy Physics - Phenomenology · Physics 2009-10-28 Mihir P. Worah

We present a generalization of a model where the right-handed up-type quarks serve as messengers for neutrino mass generation and as a portal for dark matter. Within this framework the Standard Model is extended with a single Majorana…

High Energy Physics - Phenomenology · Physics 2014-11-26 John N. Ng , Alejandro de la Puente

We demonstrate viability of the one-loop neutrino mass mechanism within the framework of grand unification when the loop particles comprise scalar leptoquarks (LQs) and quarks of the matching electric charge. This mechanism can be…

High Energy Physics - Phenomenology · Physics 2017-08-02 Ilja Doršner , Svjetlana Fajfer , Nejc Košnik

We propose a minimal one-loop radiative framework for Dirac neutrino mass matrix. As a consequence, the Yukawa hierarchies among the SM fermions are alleviated, and radiative type-I seesaw framework is realized. To regulate divergent loop…

High Energy Physics - Phenomenology · Physics 2026-03-17 Takaaki Nomura , Hiroshi Okada , Yoshihiro Shigekami

A new model for tiny neutrino masses is proposed in the gauge theory of $SU(3)_C \otimes SU(3)_L \otimes U(1)_X$, where neutrino masses are generated via the quantum effect of new particles. In this model, the fermion content is taken to be…

High Energy Physics - Phenomenology · Physics 2020-05-15 Arindam Das , Kazuki Enomoto , Shinya Kanemura , Kei Yagyu

Leptoquarks have been proposed as a possible explanation of anomalies in $\bar{B}\mapsto D^{*} \tau \bar{\nu } $ decays, the apparent anomalies in $(g-2)_\mu$ experiments and a violation of lepton universality. Motivated by this, we examine…

High Energy Physics - Phenomenology · Physics 2017-09-13 Oleg Popov , Graham A White

Models of radiative Majorana neutrino masses require new scalars and/or fermions to induce lepton number violating interactions. We show that these new particles also generate observable neutrino nonstandard interactions (NSI) with matter.…

High Energy Physics - Phenomenology · Physics 2020-03-06 K. S. Babu , P. S. Bhupal Dev , Sudip Jana , Anil Thapa

We discuss the simplest mechanisms for generating neutrino masses at tree level and one loop level. We find a significant number of new possibilities where one can generate neutrino masses at the one-loop level by adding only two new types…

High Energy Physics - Phenomenology · Physics 2009-09-09 Pavel Fileviez Perez , Mark B. Wise

We introduce two scalar leptoquarks, the SU$(2)_L$ isosinglet denoted $\phi\sim(\mathbf{3}, \mathbf{1}, -1/3)$ and the isotriplet $\varphi\sim(\mathbf{3}, \mathbf{3}, -1/3)$, to explain observed deviations from the standard model in…

High Energy Physics - Phenomenology · Physics 2019-10-17 Innes Bigaran , John Gargalionis , Raymond R. Volkas

Weak bases of flavors (u, c), (d,s), (e, \mu), (\nu_e,\nu_\mu) are assumed as the S_3 doublet and t, b, \tau, {\nu_\tau} are the S_3 singlet and further there are assumed S_3 doublet Higgs (H_1, H_2) and S_3 singlet Higgs H_S. We suggest an…

High Energy Physics - Phenomenology · Physics 2011-08-08 Tadayuki Teshima , Yoshitaka Okumura

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 simple phenomenological model of quarks-leptons mass matrices having fundamentally universal symmetry structure. These mass matrices consist of democratic and semi-democratic mass matrix terms commonly to the neutrino and the…

High Energy Physics - Phenomenology · Physics 2016-01-20 Hiroyuki Nishiura , Takeshi Fukuyama

A minimal extension of the standard model to naturally generate small neutrino masses and provide a dark matter candidate is proposed. The dark matter particle is part of a new scalar doublet field that plays a crucial role in radiatively…

High Energy Physics - Phenomenology · Physics 2014-07-03 Michael Gustafsson , Jose Miguel No , Maximiliano A. Rivera

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 suggest an approach to explain the observed pattern of the neutrino masses and mixing which employs the weakly broken quark-lepton symmetry and does not require introduction of an ad hoc symmetry of the neutrino sector. The mass matrices…

High Energy Physics - Phenomenology · Physics 2009-11-10 I. Dorsner , A. Yu. Smirnov