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We propose a new mechanism of baryogenesis which proceeds via a CP-violating phase transition. During this phase transition, the coupling of the Weinberg operator is dynamically realised and subsequently a lepton asymmetry is generated via…

High Energy Physics - Phenomenology · Physics 2017-04-28 Silvia Pascoli , Jessica Turner , Ye-Ling Zhou

We present an S$_4$ flavour symmetric model within a minimal seesaw framework resulting in mass matrices that leads to TM$_1$ mixing. Minimal seesaw is realized by adding two right-handed neutrinos to the Standard Model. The model predicts…

High Energy Physics - Phenomenology · Physics 2021-12-22 Bikash Thapa , Ng. K. Francis

We consider leptogenesis in a left-right-symmetric seesaw scenario in which neutrino mass generation and leptogenesis are dominated by the type-II seesaw term. Motivated by grand unification, we assume that the neutrino Dirac mass matrix is…

High Energy Physics - Phenomenology · Physics 2021-09-29 Thomas Rink , Werner Rodejohann , Kai Schmitz

We consider an extension of the Standard Model with three right-handed neutrinos, endowed with a flavour symmetry $G_f$, $G_f=\Delta (3 \, n^2)$ or $G_f=\Delta (6 \, n^2)$, $n \geq 2$, and CP. For large active-sterile mixing, we study the…

High Energy Physics - Phenomenology · Physics 2024-12-16 Marco Drewes , Yannis Georis , Claudia Hagedorn , Juraj Klaric

In the context of the minimal supersymmetric seesaw model, we study the implications of the current neutrino data for thermal leptogenesis, $\beta\beta_{0\nu}$ decay, and leptonic flavour- and CP-violating low-energy observables. We express…

High Energy Physics - Phenomenology · Physics 2009-09-11 John Ellis , Martti Raidal

Thermal leptogenesis, in the seesaw model, is a popular mechanism for generating the Baryon Asymmetry of the Universe. It was noticed recently, that including lepton flavour can modify significantly the results. These proceedings aim to…

High Energy Physics - Phenomenology · Physics 2007-05-23 Sacha Davidson

Viable neutrino and charged lepton masses and mixings are obtained by imposing a $S_3 \times Z_4 \times Z_3$ flavor symmetry in a model with a few additional Higgs. We use two $SU(2)_L$ triplet Higgs which are arranged as a doublet of…

High Energy Physics - Phenomenology · Physics 2008-12-30 Manimala Mitra , Sandhya Choubey

Recent observations for a non-zero $\theta_{13}$ have come from various experiments. We study a model of lepton mixing with a 2-3 flavor symmetry to accommodate the sizable $\theta_{13}$ measurement. In this work, we derive deviations from…

High Energy Physics - Phenomenology · Physics 2015-03-19 Ahmed Rashed

We present a review of neutrino phenomenology in the minimal seesaw model (MSM), an economical and intriguing extension of the Standard Model with only two heavy right-handed Majorana neutrinos. Given current neutrino oscillation data, the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wan-lei Guo , Zhi-zhong Xing , Shun Zhou

We study baryogenesis via leptogenesis in an extension of the Standard Model by adding one right-handed neutrino and one triplet scalar. These heavy particles contribute to the generation of tiny neutrino mass through seesaw mechanism. The…

High Energy Physics - Phenomenology · Physics 2023-06-28 Sreerupa Chongdar , Sasmita Mishra

We analyze lepton asymmetry induced in the decay of right--handed neutrinos in a class of minimal left--right symmetric models. In these models, which assume low energy supersymmetry, the Dirac neutrino mass matrix is proportional to the…

High Energy Physics - Phenomenology · Physics 2015-06-25 K. S. Babu , A. Bachri , H. Aissaoui

We investigate the relation between non-unitarity of the leptonic mixing matrix and leptogenesis. We discuss how all parameters of the canonical type-I seesaw mechanism can, in principle, be reconstructed from the neutrino mass matrix and…

High Energy Physics - Phenomenology · Physics 2011-05-23 Stefan Antusch , Steve Blanchet , Mattias Blennow , Enrique Fernandez-Martinez

We present a low-scale type-I seesaw scenario with discrete flavor and CP symmetries. This scenario not only explains the measured values of the lepton mixing angles, but also makes predictions for leptonic CP violation, and connects the…

High Energy Physics - Phenomenology · Physics 2023-01-03 Garv Chauhan , P. S. Bhupal Dev

We consider a type-I seesaw framework with a flavour symmetry from the series of non-abelian groups $\Delta (3 n^2)$ and $\Delta (6 n^2)$ and a CP symmetry. Breaking these symmetries non-trivially results in the right-handed neutrinos being…

High Energy Physics - Phenomenology · Physics 2022-12-20 Marco Drewes , Yannis Georis , Claudia Hagedorn , Juraj Klarić

We have shown that non-zero U_{e3} is generated in a see-saw type softly broken A_4 symmetric model through a single parameter perturbation in m_D in a single element. We have explored all possible 9 cases to study the neutrino mixing…

High Energy Physics - Phenomenology · Physics 2008-11-26 Biswajit Adhikary , Ambar Ghosal

We study the possibility of generating non-zero reactor mixing angle $\theta_{13}$ by perturbing the $\mu-\tau$ symmetric neutrino mass matrix. The leading order $\mu-\tau$ symmetric neutrino mass matrix originates from type I seesaw…

High Energy Physics - Phenomenology · Physics 2015-06-22 Manikanta Borah , Debasish Borah , Mrinal Kumar Das , Sudhanwa Patra

We give analytic approximations to the baryon asymmetry produced by thermal leptogenesis with hierarchical right-handed neutrinos. Our calculation includes flavour-dependent washout processes and CP violation in scattering, and neglects…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Abada , S. Davidson , A. Ibarra , F. -X. Josse-Michaux , M. Losada , A. Riotto

In the literature, the neutrino $\mu$-$\tau$ reflection symmetry (which has the interesting predictions $\theta^{}_{23} =\pi/4$ and $\delta = \pm \pi/2$ for the atmospherical neutrino mixing angle and Dirac CP phase) is an attractive and…

High Energy Physics - Phenomenology · Physics 2025-02-14 Yan Shao , Zhen-hua Zhao

Current experimental data allow the zero value for one neutrino mass, either m_1 = 0 or m_3 = 0. This observation implies that a realistic neutrino mass texture can be established by starting from the limit (a) m_1 = m_2 = 0 and m_3 \neq 0…

High Energy Physics - Phenomenology · Physics 2008-11-26 Aik Hui Chan , Harald Fritzsch , Shu Luo , Zhi-zhong Xing

Thermal leptogenesis, that can be viewed as a consequence of the seesaw model, is a very natural mechanism to explain the matter anti-matter asymmetry of the Universe. Recently, lepton flavours have been included in the Boltzmann equations,…

High Energy Physics - Phenomenology · Physics 2007-10-11 F. X. Josse-Michaux