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Related papers: Baryogenesis via Leptogenesis in Adjoint SU(5)

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It is shown that the requirement of preservation of baryon asymmetry does not rule out a scale for leptogenesis as low as 10 TeV. The conclusions are compatible with see-saw mechanism if for example the pivot mass scale for neutrinos is…

High Energy Physics - Phenomenology · Physics 2009-11-10 Narendra Sahu , Urjit A. Yajnik

Left-right symmetric models which employ a generalized seesaw mechanism to generate quark and charged lepton masses are known to solve the strong CP problem via parity symmetry, without the need for the axion. These models lead to naturally…

High Energy Physics - Phenomenology · Physics 2025-07-23 K. S. Babu , Ajay Kaladharan

We study the baryogenesis via leptogenesis in a class of left-right symmetric models, in which $D$-parity is broken spontaneously. We first discuss the consequence of the spontaneous $D$-parity breaking on the neutrino masses. Than we study…

High Energy Physics - Phenomenology · Physics 2009-11-11 Narendra Sahu , Utpal Sarkar

A simple model is constructed based on the gauge symmetry $SU(3)_c \times SU(2)_L \times U(1)_Y \times SU(2)_\ell$, with only the leptons transforming nontrivially under $SU(2)_\ell$. The extended symmetry is broken down to the Standard…

High Energy Physics - Phenomenology · Physics 2017-06-14 Bartosz Fornal

The minimal flipped $SU(5)$ unification with the right-handed neutrino Majorana mass scale generated as a two-loop effect is arguably one of the most constrained models of perturbative baryon and lepton number violation currently on the…

High Energy Physics - Phenomenology · Physics 2025-07-01 Michal Malinský , Renato Fonseca , Václav Miřátský , Martin Zdráhal

Leptogenesis constitues a very simple scenario to achieve the baryon asymmetry that we observe today. It requires only the presence of right handed neutrinos (which arise very naturally in many extensions of the Standard Model) and depends…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. Peloso

The cosmological baryon asymmetry can be explained by the nonperturbative electroweak reprocessing of a lepton asymmetry generated in the out-of-equilibrium decay of heavy right-handed Majorana neutrinos. We analyze this mechanism in detail…

High Energy Physics - Phenomenology · Physics 2007-05-23 Michael Pluemacher

Extending the Standard Model with right-handed neutrinos provides a minimal explanation for both light neutrino masses (through the type-I seesaw mechanism) and the baryon asymmetry of our universe (through leptogenesis). We map here for…

High Energy Physics - Phenomenology · Physics 2023-05-12 Yannis Georis

We study constraints on neutrino properties from texture zeros in bi-large mixing See-Saw mass matrix and also from leptogenesis. Texture zeros may occur in the light (class a)) or in the heavy (class b)) neutrino mass matrices. Each of…

High Energy Physics - Phenomenology · Physics 2008-11-26 Wei Chao , Xiao-Gang He , Xue-Qian Li

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

Leptogenesis is a class of scenarios where the baryon asymmetry of the Universe is produced from a lepton asymmetry generated in the decays of a heavy sterile neutrino. We explain the motivation for leptogenesis. We review the basic…

High Energy Physics - Phenomenology · Physics 2008-11-26 Sacha Davidson , Enrico Nardi , Yosef Nir

In a $U(1)_{R-L}$-symmetric supersymmetric model, pseudo-Dirac bino and wino can act like right-handed neutrinos, generating the light neutrino masses through a hybrid Type I + III inverse seesaw mechanism. We investigate such a model to…

High Energy Physics - Phenomenology · Physics 2026-01-01 Cem Murat Ayber , Tammi Chowdhury , Seyda Ipek

We consider a model with three right-handed neutrinos in which Yukawa coupling constants and Majorana masses are obtained by requiring the modular $A_4$ symmetry. It has been shown that the model can explain mass hierarchies and mixing…

High Energy Physics - Phenomenology · Physics 2021-06-01 Takehiko Asaka , Yongtae Heo , Takuya H. Tatsuishi , Takahiro Yoshida

We bring the theoretical issue of whether two important cosmological demands, baryon asymmetry and degenerate neutrinos as hot dark matter, can be compatible in the context of the seesaw mechanism. To realize leptogenesis with almost…

High Energy Physics - Phenomenology · Physics 2009-10-31 Eung Jin Chun , Sin Kyu Kang

We discuss baryogenesis using the flipped $SU(5)$ model for lepton mass matrices. We show that the generalized see-saw mechanism in this model can not only provide MSW neutrino mixing suitable for solving the solar neutrino problem, and…

High Energy Physics - Phenomenology · Physics 2009-09-11 J. Ellis , D. V. Nanopoulos , K. Olive

We consider leptogenesis in a minimal S_3 extension of the standard model with an additional Z_2 symmetry in the leptonic sector. It is found that the CP phase appearing in the neutrino mixing is the same as that for the CP asymmetries…

High Energy Physics - Phenomenology · Physics 2016-09-06 Takeshi Araki , Jisuke Kubo , Emmanuel A. Paschos

We provide the first systematic study of the viable parameter space for leptogenesis in the type-I seesaw model with three right-handed neutrinos whose Majorana masses lie below the electroweak scale. We highlight the very rich…

High Energy Physics - Phenomenology · Physics 2019-05-01 Michele Lucente , Asmaa Abada , Giorgio Arcadi , Valerie Domcke , Marco Drewes , Juraj Klaric

We propose an alternative mechanism for leptogenesis at the electroweak scale, through the decays of a left-handed sneutrino. This scenario may be realized in supersymmetric models with non-zero Majorana masses for the neutrino superfield…

High Energy Physics - Phenomenology · Physics 2007-05-23 John Ellis , Sin Kyu Kang

The presently available information on neutrino oscillations can be used to tightly constrain the light neutrino mass matrix $m_\n$ under the assumption that the three known neutrinos provide explanation of the solar and atmospheric…

High Energy Physics - Phenomenology · Physics 2007-05-23 Anjan S. Joshipura , Emmanuel A. Paschos

We propose a new scenario for baryogenesis through leptogenesis, where the CP phase relevant for leptogenesis is connected directly to the PMNS phase(s) in the light neutrino mixing matrix. The scenario is realized in case only one CP phase…

High Energy Physics - Phenomenology · Physics 2016-09-14 Laura Covi , Jihn E. Kim , Bumseok Kyae , Soonkeon Nam
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