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If the present baryon-asymmetry is due to a Planck or GUT-scale matter asymmetry then baryon- or lepton-number violating processes are constrained by the condition that they do not subsequently erase this asymmetry. We present a revision of…

High Energy Physics - Phenomenology · Physics 2009-10-22 Herbert Dreiner , Graham G. Ross

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

I show that a cosmological baryon asymmetry generated at the GUT scale is in general safe against washout due to sphalerons and generic $B$- or $L$-violating effects. This result is mainly due to the (almost) conserved number of…

High Energy Physics - Phenomenology · Physics 2010-11-01 Kimmo Kainulainen

We show that a cosmological baryon asymmetry generated at the GUT scale, which would be destroyed at lower temperatures by sphalerons and possible new B- or L-violating effects, can naturally be preserved by an asymmetry in the number of…

High Energy Physics - Phenomenology · Physics 2009-09-15 J. M. Cline , K. Kainulainen , K. A. Olive

We consider the evolution of baryon number $B$ in the early universe under the influence of rapid sphaleron interactions and show that $B$ will remain nonzero at all times even in the case of $B-L = 0$. This result arises due to thermal…

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

In this work, we classify all the effective $U(1)$ symmetries and their associated Noether charges in the Standard Model (SM) and its minimal supersymmetric extension (MSSM) from the highest scale after inflation down to the weak scale. We…

High Energy Physics - Phenomenology · Physics 2021-08-26 Chee Sheng Fong

We study the possibility of generating the observed baryon asymmetry via leptogenesis in the decay of heavy Standard Model singlet fermions which carry lepton number, in a framework without Majorana masses above the electroweak scale. Such…

High Energy Physics - Phenomenology · Physics 2009-12-14 M. C. Gonzalez-Garcia , J. Racker , N. Rius

We review the current status of baryogenesis with emphasis on electroweak baryogenesis and leptogenesis. The first detailed studies were carried out for SU(5) GUT models where CP-violating decays of leptoquarks generate a baryon asymmetry.…

High Energy Physics - Phenomenology · Physics 2021-11-09 Dietrich Bodeker , Wilfried Buchmuller

We reconsider the GUT-baryogenesis mechanism for generating the baryon asymmetry of the Universe. The baryon asymmetry is produced by the out of equilibrium decay of coloured Higgs bosons at the GUT scale, conserving B-L. If neutrinos are…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. A. Lopez-Perez , N. Rius

Using lattice simulations, we measure the sphaleron rate in the Standard Model as a function of temperature through the electroweak cross-over, for the Higgs masses m_H=115 and m_H=160 GeV. We pay special attention to the shutting off of…

High Energy Physics - Phenomenology · Physics 2012-09-04 Michela D'Onofrio , Kari Rummukainen , Anders Tranberg

We study in detail the mechanism of baryon and lepton asymmetry generation in the framework of the $\nu$MSM (an extension of the Standard Model by three singlet fermions with masses smaller than the electroweak scale). We elucidate the…

High Energy Physics - Phenomenology · Physics 2008-11-26 Mikhail Shaposhnikov

We measure the sphaleron rate with the physical parameters of the Standard Model. In particular, we plug into the calculations the recently found Higgs mass m_H = 125 GeV. The sphaleron rate tells us about the efficiency of baryon number…

High Energy Physics - Phenomenology · Physics 2012-12-14 Michela D'Onofrio , Kari Rummukainen , Anders Tranberg

In the supersymmetric standard model of particle interactions, R-parity nonconservation is often invoked to obtain nonzero neutrino masses. We point out here that such interactions of the supersymmetric particles would erase any…

High Energy Physics - Phenomenology · Physics 2009-11-19 Ernest Ma , Martti Raidal , Utpal Sarkar

The electroweak sphaleron process breaks the baryon number conservation within the realms of the Standard Model of particle physics (SM). Recently, it is pointed out that its decoupling may provide the out-of-equilibrium condition required…

High Energy Physics - Phenomenology · Physics 2024-06-18 Muzi Hong , Kohei Kamada , Jun'ichi Yokoyama

In the standard model and most of its extensions the electroweak transition is too weak to affect the cosmological baryon asymmetry. Due to sphaleron processes baryogenesis in the high-temperature, symmetric phase of the standard model is…

High Energy Physics - Phenomenology · Physics 2007-05-23 W. Buchmüller

We use large-scale lattice simulations to compute the rate of baryon number violating processes (the sphaleron rate), the Higgs field expectation value, and the critical temperature in the Standard Model across the electroweak phase…

High Energy Physics - Phenomenology · Physics 2014-10-06 Michela D'Onofrio , Kari Rummukainen , Anders Tranberg

We discuss the relation between lepton number violation at high and low energies, particularly, the constraints on baryogenesis models, which would be implied by an observation of neutrinoless double beta decay. The primordial baryon…

High Energy Physics - Phenomenology · Physics 2016-05-05 Lukas Graf

Low-scale leptogenesis provides an economic and testable description of the origin of the baryon asymmetry of the Universe. In this scenario, the baryon asymmetry of the Universe is reprocessed from the lepton asymmetry by electroweak…

High Energy Physics - Phenomenology · Physics 2017-12-06 S. Eijima , M. Shaposhnikov , I. Timiryasov

We present a new scenario for the baryon number violation that may take place in models with large extra dimensions. Our idea is interesting because leptogenesis with a low reheating temperature requires an alternative source of the B+L…

High Energy Physics - Phenomenology · Physics 2009-11-07 Tomohiro Matsuda

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
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