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Related papers: Axiogenesis from $SU(2)_R$ phase transition

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We have shown that the $B-L$ generation due to the decay of the thermally produced superheavy fields can explain the Baryon assymmetry in the universe if the superheavy fields are heavier than $10^{13-14}$ GeV. Note that although the…

High Energy Physics - Phenomenology · Physics 2013-05-29 Seishi Enomoto , Nobuhiro Maekawa

The baryon asymmetry of the universe can be explained by the out-of-equilibrium decays of heavy right-handed neutrinos. We analyse this mechanism in the framework of a supersymmetric extension of the Standard Model and show that lepton…

High Energy Physics - Phenomenology · Physics 2016-09-06 M. Plumacher

We propose that the baryon asymmetry of the Universe may originate from the amplification of quantum fluctuations of a light complex scalar field during inflation. CP-violation is sourced by complex mass terms, which are smaller than the…

Astrophysics · Physics 2008-12-18 Bjorn Garbrecht , Tomislav Prokopec

We propose a novel framework where baryon asymmetry can arise due to forbidden decay of dark matter (DM) enabled by finite temperature effects in the early universe. In order to implement it in a realistic setup, we consider the DM to be a…

High Energy Physics - Phenomenology · Physics 2023-09-06 Debasish Borah , Suruj Jyoti Das , Rishav Roshan

We show that the baryon asymmetry of the universe can be explained in models where the Higgs couples to the Chern-Simons term of the hypercharge group and is away from the late-time minimum of its potential during inflation. The Higgs then…

High Energy Physics - Phenomenology · Physics 2021-09-07 Yann Cado , Benedict von Harling , Eduard Masso , Mariano Quiros

We develop a unified model of darkgenesis and baryogenesis involving strongly interacting dark quarks, utilizing the gravitational anomaly of chiral gauge theories. In these models, both the visible and dark baryon asymmetries are generated…

High Energy Physics - Theory · Physics 2018-10-12 Stephon Alexander , Evan McDonough , David N. Spergel

Non-supersymmetric Grand Unified $SO(10)\times U(1)_{\rm PQ}$ models have all the ingredients to solve several fundamental problems of particle physics and cosmology -- neutrino masses and mixing, baryogenesis, the non-observation of strong…

High Energy Physics - Phenomenology · Physics 2018-05-08 Anne Ernst , Andreas Ringwald , Carlos Tamarit

We construct a model based on an extra gauge symmetry, SU(2)_X x U(1)_{B-L}, which can provide gauge bosons to serve as weakly-interacting massive particle dark matter. The stability of the dark matter is naturally guaranteed by a discrete…

High Energy Physics - Phenomenology · Physics 2014-03-07 Cheng-Wei Chiang , Takaaki Nomura , Jusak Tandean

We investigate that the two types of the Q balls explain the baryon asymmetry and the dark matter of the universe in the gauge-mediated supersymmetry breaking. The gauge-mediation type Q balls of one flat direction produce baryon asymmetry,…

High Energy Physics - Phenomenology · Physics 2015-06-18 Shinta Kasuya , Masahiro Kawasaki

We introduce a model for matters-genesis in which both the baryonic and dark matter asymmetries originate from a first-order phase transition in a dark sector with an $SU(3)\times SU(2)\times U(1)$ gauge group and minimal matter content. In…

High Energy Physics - Phenomenology · Physics 2023-03-10 Eleanor Hall , Thomas Konstandin , Robert McGehee , Hitoshi Murayama

We consider a setup where R-parity is violated in the framework of split supersymmetry. The out-of-equilibrium decays of heavy squarks successfully lead to the generation of a baryon asymmetry. We restrict the R-parity violating couplings…

High Energy Physics - Phenomenology · Physics 2009-11-11 Stephan J. Huber

We propose a minimal extension of the standard model with U(1)_{B-L} \times Z_{2} symmetry. In this model by assuming that the neutrinos are Dirac (i.e. $B-L$ is an exact symmetry), we found a simultaneous solution for non zero neutrino…

High Energy Physics - Phenomenology · Physics 2018-10-17 Nimmala Narendra , Nirakar Sahoo , Narendra Sahu

In the presence of anomaly induced sphaleron process, only a B-L asymmetry can be partially converted to the baryon asymmetry while any B+L asymmetry would be completely erased. Thus in any successful baryogenesis theories, B-L is usually…

High Energy Physics - Phenomenology · Physics 2008-11-26 Pei-Hong Gu , Utpal Sarkar

We present a simple mechanism which allows the simultaneous generation of the baryon asymmetry of the Universe along with its dark matter content. To this goal, we employ the out-of-equilibrium decays of heavy bath states into a feebly…

High Energy Physics - Phenomenology · Physics 2022-02-17 Andreas Goudelis , Pantelis Papachristou , Vassilis C. Spanos

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 propose an extension of the Standard Model in which baryon number is promoted to be part of a non-Abelian gauge symmetry at high energies. Specifically, we consider the gauge group SU(4) x SU(2)_L x U(1)_X, where the SU(4) unifies baryon…

High Energy Physics - Phenomenology · Physics 2015-09-23 Bartosz Fornal , Arvind Rajaraman , Tim M. P. Tait

We propose a mechanism called sphalerogenesis to explain the baryon asymmetry of the universe (BAU). The BAU is explained by a CP-violating decay of the electroweak sphaleron. We introduce a dimension-six operator constructed from weak…

High Energy Physics - Phenomenology · Physics 2026-05-05 Masanori Tanaka

We present a mechanism to generate the baryon asymmetry of the Universe which preserves the net baryon number created in the Big Bang. If dark matter particles carry baryon number $B_X$, and $\sigma^{\rm annih}_{\bar{X}} < \sigma^{\rm…

High Energy Physics - Phenomenology · Physics 2007-05-23 Glennys R. Farrar , Gabrijela Zaharijas

The cosmological matter-antimatter asymmetry can arise from the baryon number conserving CP asymmetry in two body decays of heavy particles, when the two final states carry equal and opposite baryon number, and one couples directly or…

High Energy Physics - Phenomenology · Physics 2014-02-12 D. Aristizabal Sierra , Chee Sheng Fong , Enrico Nardi , Eduardo Peinado

We show that grand unified theories based on SO(10) generate quite naturally baryon number violating dimension seven operators that violate (B-L), and lead to novel nucleon decay modes such as n \to e^-K^+, e^- \pi^+ and p \to \nu \pi^+. We…

High Energy Physics - Phenomenology · Physics 2015-06-05 K. S. Babu , R. N. Mohapatra
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