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Related papers: Aidnogenesis via Leptogenesis and Dark Sphalerons

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The observed dark matter relic abundance may be explained by different mechanisms, such as thermal freeze-out/freeze-in, with one or more symmetric/asymmetric components. In this work we investigate the role played by asymmetries in…

High Energy Physics - Phenomenology · Physics 2023-05-15 Juan Herrero-Garcia , Giacomo Landini , Drona Vatsyayan

I suggest an extension of the SM by introducing a dark sector with the local $U(1)_{D}$ symmetry. The particles in the dark sector bring about the new physics beyond the SM. In particular the global $B-L$ symmetry is violated just above the…

High Energy Physics - Phenomenology · Physics 2017-08-25 Wei-Min Yang

I suggest a new extension of the standard model of particle physics, which introduces a dark sector with the $SU(2)_{D}\otimes U(1)_{D'}$ symmetry besides the SM sector. The new particles of the model all inhabit in the dark sector. The…

High Energy Physics - Phenomenology · Physics 2019-06-26 Wei-Min Yang

It is proposed that dark matter is the origin of neutrino mass, thereby linking inexorably two undisputed (and seemingly unrelated) pieces of evidence for physics beyond the Standard Model. Leptogenesis at the TeV scale may also be…

High Energy Physics - Phenomenology · Physics 2008-11-26 Ernest Ma

Asymmetric Dark Matter (ADM) models invoke a particle-antiparticle asymmetry, similar to the one observed in the Baryon sector, to account for the Dark Matter (DM) abundance. Both asymmetries are usually generated by the same mechanism and…

High Energy Physics - Phenomenology · Physics 2015-06-04 Mattias Blennow , Enrique Fernandez-Martinez , Olga Mena , Javier Redondo , Paolo Serra

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

We evaluate the constraints that the COBE observations put on baryogenesis in inflationary cosmologies.We consider the supersymmetric version of the proposal of Fukugita and Yanagida, that the baryon asymmetry of the universe is created by…

High Energy Physics - Phenomenology · Physics 2009-09-15 B. A. Campbell , S. Davidson , K. A. Olive

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 W. Buchmuller , M. Plumacher

We consider the singlet Majoron model with softly broken lepton number. This model contains three right-handed neutrinos and a singlet scalar besides the standard model fields. The real part of the singlet scalar develops a vacuum…

High Energy Physics - Phenomenology · Physics 2014-11-20 Pei-Hong Gu , Ernest Ma , Utpal Sarkar

In an unconventional realization of left-right symmetry, the particle corresponding to the left-handed neutrino nu_L (with SU(2)_L interactions) in the right-handed sector, call it n_R (with SU(2)_R interactions), is not its Dirac mass…

High Energy Physics - Phenomenology · Physics 2015-06-04 Ernest Ma

We present a simple extension of the standard model that gives rise to baryogenesis a has a dark matter candidate of O(GeV) mass. A minimal set of new fields required for baryogenesis includes two O(TeV) colored scalars and a singlet…

High Energy Physics - Phenomenology · Physics 2013-08-09 Rouzbeh Allahverdi , Bhaskar Dutta

The lepton asymmetry created in the out-of-equilibrium decay of a heavy Majorana neutrino can generate the cosmological baryon asymmetry when processed through fast anomalous electroweak reactions. In this work I examine this process under…

High Energy Physics - Phenomenology · Physics 2014-11-17 Haim Goldberg

We propose a new mechanism of leptogenesis in which the asymmetries in lepton numbers are produced through the CP-violating oscillations of ``sterile'' (electroweak singlet) neutrinos. The asymmetry is communicated from singlet neutrinos to…

High Energy Physics - Phenomenology · Physics 2008-11-26 E. Kh. Akhmedov , V. A. Rubakov , A. Yu. Smirnov

We propose an extended version of the standard model, in which neutrino oscillation, dark matter, and baryon asymmetry of the Universe can be simultaneously explained by the TeV-scale physics without assuming unnatural hierarchy among the…

High Energy Physics - Phenomenology · Physics 2009-02-27 Mayumi Aoki , Shinya Kanemura , Osamu Seto

The rates for generating a matter-antimatter asymmetry in extensions of the Standard Model (SM) containing right-handed neutrinos are the most interesting and least trivial coefficients in the rate equations for baryogenesis through thermal…

High Energy Physics - Phenomenology · Physics 2017-07-05 Dietrich Bodeker , Marc Sangel

Leptogenesis is a class of scenarios in which the cosmic baryon asymmetry originates from an initial lepton asymmetry generated in the decays of heavy sterile neutrinos in the early Universe. We explain why leptogenesis is an appealing…

High Energy Physics - Phenomenology · Physics 2013-01-16 Chee Sheng Fong , Enrico Nardi , Antonio Riotto

A mechanism for leptogenesis at the electroweak scale was investigated in a model of dark energy and dark matter proposed by one of us (PQH). This model involves an asymptotically free gauge group SU(2)Z and an axion-like particle with an…

High Energy Physics - Phenomenology · Physics 2010-04-23 Huicheng Guo , P. Q. Hung

Instead of creating the observed baryon asymmetry of the universe by the decay of right-handed (RH) neutrinos to left-handed leptons, we propose to generate it dominantly by the decay of the RH neutrinos to RH leptons. This mechanism turns…

High Energy Physics - Phenomenology · Physics 2009-11-11 Michele Frigerio , Thomas Hambye , Ernest Ma

We study leptogenesis in two seesaw models where maximal atmospheric neutrino mixing and $U_{e3} = 0$ result from symmetries. Salient features of those models are the existence of three Higgs doublets and a twofold degeneracy of the…

High Energy Physics - Phenomenology · Physics 2009-11-10 W. Grimus , L. Lavoura

We consider a baryogenesis scenario, where the difference of baryon (B) and lepton (L) number is conserved in such a way that the B-L asymmetry in the standard model sector is compensated by an asymmetry of opposite sign stored in the dark…

High Energy Physics - Phenomenology · Physics 2010-11-26 Florian Bauer , Marc-Thomas Eisele , Mathias Garny
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