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

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We perform a systematic study of the Dirac neutrino masses which arise from a dimension five effective operator with a singlet scalar. We identify all possible realizations of this operator at tree level and one-loop level. The…

High Energy Physics - Phenomenology · Physics 2018-06-06 Chang-Yuan Yao , Gui-Jun Ding

We present a model of radiative neutrino mass that automatically contains an accidental $Z_2$ symmetry and thus provides a stable dark matter candidate. This allows a common framework for the origin of neutrino mass and dark matter without…

High Energy Physics - Phenomenology · Physics 2015-11-10 Amine Ahriche , Kristian L. McDonald , Salah Nasri , Takashi Toma

We study a $U(1)_{B-L}$ extension of the Standard Model (SM) in which Dirac neutrino masses are generated radiatively at the one-loop level through the exchange of new beyond the SM fields. This framework establishes a direct connection…

High Energy Physics - Phenomenology · Physics 2026-01-28 Chayan Majumdar , Utkarsh Patel , Supriya Senapati , Sudhanwa Patra

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

We propose an extension of the Standard Model (SM) for radiative neutrino mass by introducing a dark $U(1)_D$ gauge symmetry. The kinetic mixing between the SM gauges and the dark $U(1)_D$ gauge arises at 1-loop mediated by new inert scalar…

High Energy Physics - Phenomenology · Physics 2021-04-20 Arnab Dasgupta , Sin Kyu Kang , Myeonghun Park

We propose a radiative lepton model, in which the charged lepton masses are generated at one-loop level, and the neutrino masses are induced at two-loop level. On the other hand, tau mass is derived at tree level since it is too heavy to…

High Energy Physics - Phenomenology · Physics 2015-06-18 Seungwon Baek , Hiroshi Okada , Takashi Toma

Choosing how gauge $U(1)_\chi$ breaks in the context of $SO(10) \to SU(5) \times U(1)_\chi$, $Z_4$ lepton number may be obtained which maintains neutrinos as Dirac fermions. Choosing $\Delta(27)$ as the family symmetry of leptons,…

High Energy Physics - Phenomenology · Physics 2019-10-02 Ernest Ma

The minimal seesaw extension of the Standard 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 light neutrino masses…

High Energy Physics - Phenomenology · Physics 2016-06-15 Roberto A. Lineros

We construct a list of minimal scale-invariant models at the TeV scale that generate one-loop neutrino mass and give viable dark matter candidates. The models generically contain a singlet scalar and a $Z_2$-odd sector comprised of singlet,…

High Energy Physics - Phenomenology · Physics 2016-09-21 Amine Ahriche , Adrian Manning , Kristian L. McDonald , Salah Nasri

We propose a model where the masses of the active neutrinos and a dark matter candidate are generated radiatively through the $U(1)_{B-L}$ gauge symmetry breaking. It is realized by a non-universal $U(1)_{B-L}$ charge assignment on the…

High Energy Physics - Phenomenology · Physics 2021-07-14 Hiroshi Okada , Yuta Orikasa , Yutaro Shoji

We present a composite scotogenic model for neutrino masses, which are generated via loops of $\mathbb{Z}_2$-odd composite scalars. We consider three different approaches to the couplings of the neutrinos (including three right-handed…

High Energy Physics - Phenomenology · Physics 2021-10-22 Giacomo Cacciapaglia , Martin Rosenlyst

We present a three-loop model of neutrino mass in which both the weak scale and neutrino mass arise as radiative effects. In this approach, the scales for electroweak symmetry breaking, dark matter, and the exotics responsible for neutrino…

High Energy Physics - Phenomenology · Physics 2016-02-11 Amine Ahriche , Kristian L. McDonald , Salah Nasri

A new realization for radiative neutrino mass generation is presented. Based on the requirement of tree-level custodial symmetry and the introduction of higher (greater than two) dimensional representations for scalar fields, a specific…

High Energy Physics - Phenomenology · Physics 2016-02-17 Alfredo Aranda , Eduardo Peinado

We construct a loop induced seesaw model in a TeV scale theory with gauged U(1)_{B-L} symmetry. Light neutrino masses are generated at two-loop level and right-handed neutrinos also obtain their masses by one-loop effect. Multi-component…

High Energy Physics - Phenomenology · Physics 2013-08-09 Yuji Kajiyama , Hiroshi Okada , Takashi Toma

The minimal Standard Model extension with the Weinberg operator does accommodate the observed neutrino masses and mixing, but predicts a neutrinoless double beta ($0\nu\beta\beta$) decay rate proportional to the effective electron neutrino…

High Energy Physics - Phenomenology · Physics 2015-06-03 Francisco del Aguila , Alberto Aparici , Subhaditya Bhattacharya , Arcadi Santamaria , Jose Wudka

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

In this work, we report on recent analyses of a class of models that generate neutrino mass at the three-loop level. We argue that these models offer a viable solution to both the neutrino mass and dark matter problems, without being in…

High Energy Physics - Phenomenology · Physics 2015-05-19 Amine Ahriche , Kristian L. McDonald , Salah Nasri

We propose a model with two Higgs doublet where quark and charged-lepton masses in the first and second families are induced at one-loop level, and neutrino masses are induced at the two-loop level. In our model we introduce an extra…

High Energy Physics - Phenomenology · Physics 2017-07-19 Takaaki Nomura , Hiroshi Okada

A mechanism of radiatively generating neutrino masses is implemented in an SU(2)_L x U(1)_Y x SU(2)'_L x U(1)'_Y model, where the first and second families respect SU(2)_L x U(1)_Y while SU(2)'_L x U(1)'_Y is specific for the third family.…

High Energy Physics - Phenomenology · Physics 2009-10-31 Yutaka Okamoto , Masaki Yasue

The radiative neutrino mass model can relate neutrino masses and dark matter at a TeV scale. If we apply this model to thermal leptogenesis, we need to consider resonant leptogenesis at that scale. It requires both finely degenerate masses…

High Energy Physics - Phenomenology · Physics 2016-03-23 Shoichi Kashiwase , Daijiro Suematsu