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Related papers: Falsifying Baryogenesis with Neutrinoless Double B…

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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

In the presence of background fields that spontaneously violate Lorentz invariance, a matter-antimatter asymmetry can be generated even in thermal equilibrium. In this paper we systematically investigate models of this type, showing that…

High Energy Physics - Phenomenology · Physics 2011-05-12 Sean M. Carroll , Jing Shu

We discuss the contributions of lepton-number-violating sources to neutrinoless double beta decay ($0\nu\beta\beta$). Assuming that these sources arise at scales well above the electroweak scale, they can be described within an effective…

High Energy Physics - Phenomenology · Physics 2019-06-13 W. Dekens

Baryon number violation is our most sensitive probe of physics beyond the Standard Model. Its realization through heavy new particles can be conveniently encoded in higher-dimensional operators that allow for model-agnostic analyses. The…

High Energy Physics - Phenomenology · Physics 2026-03-19 Julian Heeck , Diana Sokhashvili , Anil Thapa

We present a study of resonant leptogenesis in a radiative seesaw model. We consider the case where two quasi-degenerate right-handed neutrinos realize resonant leptogenesis, and the CP violation necessary to achieve leptogenesis occurs…

High Energy Physics - Phenomenology · Physics 2023-01-11 Bikash Thapa , Ng. K. Francis

We point out two simple but instructive possibilities to construct the charged lepton and neutrino mass matrices, from which the nearly bi-maximal neutrino mixing with large T violation can naturally emerge. The two lepton mixing scenarios…

High Energy Physics - Phenomenology · Physics 2014-11-17 Zhi-zhong Xing

We propose a novel leptogenesis scenario at the reheating era. Our setup is minimal in the sense that, in addition to the standard model Lagrangian, we only consider an inflaton and higher dimensional operators. The lepton number asymmetry…

High Energy Physics - Phenomenology · Physics 2016-11-10 Yuta Hamada , Kiyoharu Kawana

We propose a baryo- and leptogenesis mechanism in which the B-L asymmetry is produced in the conversion of ordinary leptons into particles of some depleted hidden sector. In particular, we consider the lepton number violating reactions, l…

High Energy Physics - Phenomenology · Physics 2009-09-25 Luis Bento , Zurab Berezhiani

We study a model for leptogenesis in which the total CP asymmetries in the decays and scatterings involving the SU(2) singlet seesaw neutrinos $N_\alpha$ vanish ($\epsilon_{N_\alpha}=0$). Leptogenesis is possible due to non-vanishing CP…

High Energy Physics - Phenomenology · Physics 2014-11-18 D. Aristizabal Sierra , Luis Alfredo Muñoz , Enrico Nardi

We propose a mechanism for hiding the primordial baryon asymmetry from interactions that could wash it out. It requires the introduction of a baryon number carrying singlet which is in equilibrium in the early universe and shares any…

High Energy Physics - Phenomenology · Physics 2009-10-28 Sacha Davidson , Ralf Hempfling

We present a proof-of-concept extension to the Standard Model that can generate a non-vanishing neutrinoless double beta decay ($0\nu\beta\beta$) signal without the existence of Majorana neutrinos or lepton number violation in the…

High Energy Physics - Phenomenology · Physics 2024-08-05 Lukáš Gráf , Sudip Jana , Oliver Scholer , Nele Volmer

Neutrinoless double beta decay is a very important process both from the particle and nuclear physics point of view. From the elementary particle point of view it pops up in almost every model. giving rise, among others, to the following…

High Energy Physics - Phenomenology · Physics 2008-11-26 J. D. Vergados

Primordial Big-Bang Nucleosynthesis (BBN) tightly constrains the existence of any additional relativistic degrees of freedom at that epoch. However a large asymmetry in electron neutrino number shifts the chemical equilibrium between the…

High Energy Physics - Phenomenology · Physics 2009-10-31 J. March-Russell , H. Murayama , A. Riotto

We present a model of leptogenesis that preserves lepton number. The model maintains the important feature of more traditional leptogenesis scenarios: the decaying particles that provide the CP violation necessary for baryogenesis also…

High Energy Physics - Phenomenology · Physics 2009-09-29 Hitoshi Murayama , Aaron Pierce

In the context of TeV-scale lepton number violating (LNV) interactions, we illustrate the interplay between leptogenesis, neutrinoless double beta ($0\nu\beta\beta$) decay, and LNV searches at proton-proton colliders. Using a concrete model…

High Energy Physics - Phenomenology · Physics 2024-07-25 Julia Harz , Michael J. Ramsey-Musolf , Tianyang Shen , Sebastián Urrutia Quiroga

We study scenarios in which the baryon asymmetry is generated from the decay of a particle whose mass originates from the spontaneous breakdown of a symmetry. This is realized in many models, including low-scale leptogenesis and theories…

High Energy Physics - Phenomenology · Physics 2017-11-22 Brian Shuve , Carlos Tamarit

We examine the generation of baryon asymmetry at the weak scale from a primordial lepton asymmetry. If the electroweak phase transition is first order, partial reflection of tau leptons off the bubble walls and the resulting hypercharge…

High Energy Physics - Phenomenology · Physics 2009-10-28 S. A. Abel , K. E. C. Benson

The motivation for the search for $0\nu\beta\beta$ decay is briefly reviewed. It is stressed that the exchange of light Majorana neutrinos is not the only possible mechanism of the decay. The link between lepton number and lepton flavor…

High Energy Physics - Phenomenology · Physics 2008-07-11 Petr Vogel

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

Baryon number ($B$) conservation underlies the apparent stability of ordinary matter by forbidding the decay of nucleons, while lepton number ($L$) conservation plays a central role in the structure of lepton interactions and the possible…

High Energy Physics - Phenomenology · Physics 2026-02-11 Volodymyr Takhistov