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Related papers: Modular $A_4$ invariance and leptogenesis

200 papers

We study a multi-localization model for charged leptons and neutrinos, including the possibility of a see-saw mechanism. This framework offers the opportunity to allow for realistic solutions in a consistent model without fine-tuning of…

High Energy Physics - Phenomenology · Physics 2009-11-10 J. -M. Frere , G. Moreau , E. Nezri

There are no upper limits on the possible number of massive, singlet (right--handed) neutrinos that may participate in the seesaw mechanism, and some string constructions motivate seesaw models with up to O(100) right--handed neutrinos. In…

High Energy Physics - Phenomenology · Physics 2008-11-26 John Ellis , Oleg Lebedev

We address the issue of the neutrino masses and mixing in TeV scale $B-L$ extension of the Standard Model. We show that if Dirac neutrino masses are of order $10^{-4}$ Gev, then the measured neutrino masses are correctly obtained. We…

High Energy Physics - Phenomenology · Physics 2011-03-23 M . Abbas , S. Khalil

During a large period of time, the anomalous baryon number violating interactions are in equilibrium, when the $(B+L)$ asymmetry is washed out. If there is any lepton number violation during this period, that will also erase the $(B-L)$…

High Energy Physics - Phenomenology · Physics 2007-05-23 Utpal Sarkar

The effects of the lightest neutrino mass in ``flavoured'' leptogenesis are investigated in the case when the CP-violation necessary for the generation of the baryon asymmetry of the Universe is due exclusively to the Dirac and/or Majorana…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Molinaro , S. T. Petcov , T. Shindou , Y. Takanishi

We study lepto-axiogenesis in theories where the right-handed neutrino is light enough that its dynamics affect the determination of the baryon asymmetry. When compared with theories of high-scale lepto-axiogenesis where the Majorana…

High Energy Physics - Phenomenology · Physics 2024-02-19 Patrick Barnes , Raymond T. Co , Keisuke Harigaya , Aaron Pierce

The baryon to photon ratio in the present Universe is very accurately measured to be $(6.065 \pm 0.090) \times 10^{-10}$. We study the possible origin of this baryon asymmetry in the neutrino sector through the generic mechanism of…

High Energy Physics - Phenomenology · Physics 2014-07-10 Debasish Borah , Mrinal Kumar Das

A beautiful understanding of the smallness of the neutrino masses may be obtained via the seesaw mechanism, whereby one takes advantage of the key qualitative distinction between the neutrinos and the other fermions: right-handed neutrinos…

High Energy Physics - Phenomenology · Physics 2015-06-03 Brian Feldstein , William Klemm

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 the see-saw mechanism for hierarchical Dirac and Majorana neutrino mass matrices m_D and M_R, including the CP violating phases. Simple arguments about the structure of the neutrino mass matrix and the requirement of successful…

High Energy Physics - Phenomenology · Physics 2011-07-19 Werner Rodejohann

Continuous $U(1)_{L_\mu-L_\tau}$ symmetry can generate quasi degenerate mass spectrum for both left handed light and right handed heavy Majorana neutrinos assuming that the symmetry preserving non zero parameters are nearly same. There is…

High Energy Physics - Phenomenology · Physics 2009-11-11 Biswajit Adhikary

We construct a model realizing the inverse seesaw mechanism. The model has two types of gauge singlet fermions in addition to right-handed neutrinos. A required Majorana mass scale (keV scale) for generating the light active neutrino mass…

High Energy Physics - Phenomenology · Physics 2015-11-30 Mayumi Aoki , Naoyuki Haba , Ryo Takahashi

Baryogenesis appears to require lepton number violation. This is naturally realized in extensions of the standard model containing right-handed neutrinos. We discuss the generation of a baryon asymmetry by the out-of-equilibrium decay of…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Plumacher

Both neutrinoless double beta decay and leptogenesis require neutrinos to be Majorana fermions. A relation between these two phenomena can be derived once the mechanism of neutrino mass generation is specified. We first derive the…

High Energy Physics - Phenomenology · Physics 2021-02-03 Nimmala Narendra , Narendra Sahu , S. Uma Sankar

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 propose a leptogenesis scenario where baryon asymmetry generation is assisted by the kinetic motion of the majoron, $J$, in the process of lepton-number violating inverse decays of a right-handed neutrino, $N$. We investigate two…

High Energy Physics - Phenomenology · Physics 2024-04-30 Eung Jin Chun , Tae Hyun Jung

We consider the possibility to detect right-handed neutrinos, which are mostly singlets of the Standard Model gauge group, at future accelerators. Substantial mixing of these neutrinos with the active neutrinos requires a cancellation of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Joern Kersten , Alexei Yu. Smirnov

We for the first time map the range of active-sterile neutrino mixing angles in which leptogenesis is possible in the type I seesaw model with three heavy neutrinos with Majorana masses between 50 MeV and 100 TeV, covering the entire…

High Energy Physics - Phenomenology · Physics 2022-02-03 Marco Drewes , Yannis Georis , Juraj Klarić

It is pointed out that if a neutrino mass matrix for right-handed neutrinos in seesaw mechanism has mu -tau symmetry and total lepton number L_{e}+L_{\mu }+L_{\tau} remains constant (not zero), exact tribimaximal neutrino mixing in this…

High Energy Physics - Phenomenology · Physics 2008-09-23 Riazuddin

The current work involves augmenting the $\Delta(54)$ discrete flavor model by incorporating two Standard Model Higgs particles into the Inverse Seesaw mechanism. We introduced Weyl fermions and Vector like fermions, which are gauge…

High Energy Physics - Phenomenology · Physics 2024-03-01 Hrishi Bora , Ng. K. Francis , Bikash Thapa , Shawan Kumar Jha