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We propose a two loop induced Dirac type neutrino model at TeV scale. Subsequently, three types of dark matter particles; fermion and two bosons, are naturally introduced. Here we discuss to analyze two possibilities; two component dark…

High Energy Physics - Phenomenology · Physics 2014-04-02 Hiroshi Okada

We explore a gauged $U(1)_{B-L}$ extension of standard model with inclusion of three right-handed neutrinos of exotic $B-L$ charges to cancel the gauge anomaly. Non-trivial transformation of new particles under $B-L$ symmetry forbids the…

High Energy Physics - Phenomenology · Physics 2022-07-13 Subhasmita Mishra , Nimmala Narendra , Prafulla Kumar Panda , Nirakar Sahoo

We explore the possibility to explain a bosonic dark matter candidate with a gauge singlet inside the loop to generate the neutrino mass matrix at two-loop level. The mass matrix is suppressed by a small mixing that comes from the bound on…

High Energy Physics - Phenomenology · Physics 2019-03-05 Seungwon Baek , Hiroshi Okada , Yuta Orikasa

We propose a new type of radiative neutrino model with a local hidden $U(1)$ symmetry, in which neutrino masses are induced at the three loop level, and discuss the muon anomalous magnetic moment, and dark matter candidates therein. By…

High Energy Physics - Phenomenology · Physics 2016-07-20 P. Ko , Takaaki Nomura , Hiroshi Okada , Yuta Orikasa

Models with spontaneously broken global lepton number can lead to a pseudo-Goldstone boson as a long-lived dark matter candidate. Here we revisit the case of singlet majoron dark matter and discuss multiple constraints. For masses above…

High Energy Physics - Phenomenology · Physics 2017-05-23 Camilo Garcia-Cely , Julian Heeck

We study a radiative seesaw model at one-loop level with a flavor dependent gauge symmetry $U(1)_{\mu-\tau}$, in which we consider bosonic dark matter. We also analyze the constraints from lepton flavor violations, muon $g-2$, relic density…

High Energy Physics - Phenomenology · Physics 2018-05-09 SangJong Lee , Takaaki Nomura , Hiroshi Okada

We study a model with $U(1)$ gauged lepton number symmetry in which the active neutrino masses are generated at two-loop level through the spontaneous breaking of the lepton number symmetry. To cancel gauge anomalies some exotic leptons are…

High Energy Physics - Phenomenology · Physics 2017-06-06 Takaaki Nomura , Hiroshi Okada

The proposed work is an extension of the Standard Model, where we have introduced two gauge symmetries, i.e., $U(1)_{B-L}$ and $U(1)_{L_e-L_\mu}$ to study neutrino phenomenology, muon, and electron $(g-2)$ as well as leptogenesis using the…

High Energy Physics - Phenomenology · Physics 2023-08-04 Papia Panda , Mitesh Kumar Behera , Priya Mishra , Rukmani Mohanta

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 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

In this study, we attempt to introduce a model to illustrate neutrino phenomenology by incorporating two right-handed fermion triplet superfields, i.e., $\Sigma_{R_j}$, in the presence of the modular symmetry $\Gamma_3^\prime \simeq…

High Energy Physics - Phenomenology · Physics 2023-06-14 Priya Mishra , Mitesh Kumar Behera , Rukmani Mohanta

The gauged $U(1)_{L_{\mu}-L_{\tau}}$ model can provide for additional contributions to the muon anomalous magnetic moment by means of a loop involving the $Z^{\prime}$ gauge boson. However, the parameter space of such models is severely…

High Energy Physics - Phenomenology · Physics 2018-11-06 Heerak Banerjee , Pritibhajan Byakti , Sourov Roy

Motivated by the long-standing tension in the muon anomalous magnetic moment (AMM) and persistent observations of B-physics anomalies in $R_{D^{(\ast)}}$ and $R_{K^{(\ast)}}$ ratios, we construct a simple two-loop radiative neutrino mass…

High Energy Physics - Phenomenology · Physics 2020-07-29 Shaikh Saad

We find constraints on the highest scale of symmetry breaking of a model with gauge symmetry $SU(3)_C \otimes SU(3)_L \otimes U(1)_X$ with heavy neutral leptons in the fermion triplets, calculating the anomalous magnetic moment of the muon…

High Energy Physics - Phenomenology · Physics 2021-03-03 C. E. Alvarez-Salazar , O. L. G. Peres

We propose a simple model to obtain sizable muon anomalous magnetic dipole moment (muon $g-2$) introducing several $SU(2)_L$ multiplet fields without any additional symmetries. The neutrino mass matrix is simply induced via type-II seesaw…

High Energy Physics - Phenomenology · Physics 2025-02-04 Takaaki Nomura , Hiroshi Okada

We propose a model where neutrino masses are generated at three loop order but neutrinoless double beta decay occurs at one loop. Thus we can have large neutrinoless double beta decay observable in the future experiments even when the…

High Energy Physics - Phenomenology · Physics 2018-06-21 Julien Alcaide , Dipankar Das , Arcadi Santamaria

We propose a two-loop radiative neutrino mass model based on the modular $\Gamma_4 \simeq S_4$ flavour symmetry supplemented by a discrete $Z_3$ symmetry. After spontaneous modular symmetry breaking, a remnant $Z_2$ symmetry guarantees both…

We consider the neutrino physics of models with a sequentially broken U(2) flavor symmetry. Such theories yield the observed pattern of quark and lepton masses, while maintaining sufficient degeneracies between superparticles of the first…

High Energy Physics - Phenomenology · Physics 2014-11-17 Christopher D. Carone , Lawrence J. Hall

We study the gauged U(1)_{B-L} extensions of the models for neutrino masses and dark matter. In this class of models, tiny neutrino masses are radiatively induced through the loop diagrams, while the origin of the dark matter stability is…

High Energy Physics - Phenomenology · Physics 2016-10-20 Shu-Yu Ho , Takashi Toma , Koji Tsumura

We demonstrate that an $SU(2)_L\times U(1)_Y$ model with the same particle content as Standard Model(SM) and discrete reflection symmetry between second and third generation of leptons give rise to charged lepton and neutrino mass matrices…

High Energy Physics - Phenomenology · Physics 2007-05-23 Ambar Ghosal