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相关论文: Turning Around the Sphaleron Bound: Electroweak Ba…

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The standard requirement for the production of baryons at the electroweak phase transition, that the phase transition be first order and the sphaleron bound be satisfied, is predicated on the assumption of a radiation dominated universe at…

高能物理 - 唯象学 · 物理学 2016-09-06 Michael Joyce

Radiation domination at the electroweak epoch is a simplifying assumption, but one for which there is no observational basis. Treating the expansion rate as a variable, I re-examine electroweak baryogenesis in various scenarios. At a first…

高能物理 - 唯象学 · 物理学 2007-05-23 Michael Joyce

We reanalyse the sphaleron bound of electroweak baryogenesis when allowing deviations to the Friedmann equation. These modifications are well motivated in the context of brane cosmology where they appear without being in conflict with major…

高能物理 - 唯象学 · 物理学 2014-11-17 G. Servant

In this study we examine post-inflationary cosmologies dominated by a scalar field with the equation of state: p_phi=w_phi rho_phi (0 leq w_phi leq 1) in order to facilitate baryogenesis at the electroweak scale. We take a more conventional…

高能物理 - 唯象学 · 物理学 2009-10-31 Tomislav Prokopec

We propose a new alternative for baryogenesis which resolves a number of the problems associated with GUT and electroweak scenarios, and which may allow baryogenesis even in modest extensions of the standard model. If the universe never…

高能物理 - 唯象学 · 物理学 2009-10-31 Lawrence M. Krauss , Mark Trodden

We present a novel scenario for baryogenesis in a hybrid inflation model at the electroweak scale, in which the Standard Model Higgs field triggers the end of inflation. One of the conditions for successful baryogenesis, the departure from…

高能物理 - 唯象学 · 物理学 2016-08-25 Juan Garcia-Bellido , Dmitri Grigoriev , Alexander Kusenko , Mikhail Shaposhnikov

We propose a mechanism for baryogenesis in which the baryon asymmetry is generated as an equilibrium response of weak sphalerons in a region where electroweak sphaleron transitions remain unsuppressed, $h/T\lesssim 1$. A nonzero equilibrium…

高能物理 - 唯象学 · 物理学 2026-05-18 Jacopo Azzola , Oleksii Matsedonskyi , Andreas Weiler

Scalar fields can play a dominant role in the dynamics of the Universe until shortly before nucleosynthesis. Examples are provided by domination by a kinetic mode of a scalar field, which may be both the inflaton and the late time…

高能物理 - 唯象学 · 物理学 2009-10-31 M. Joyce , T. Prokopec

A cosmological pseudoscalar field coupled to hypercharge topological number density can exponentially amplify hyperelectric and hypermagnetic fields while coherently rolling or oscillating, leading to the formation of a time-dependent…

高能物理 - 唯象学 · 物理学 2009-10-31 Ram Brustein , David H. Oaknin

The origin of the matter-antimatter asymmetry remains one of the most fundamental problems of cosmology. In this talk I present a novel scenario for baryogenesis at the electroweak scale, without the need for a first order phase transition.…

高能物理 - 唯象学 · 物理学 2016-11-03 Juan Garcia-Bellido

We study the possibility of relaxing the cosmological bound on the Higgs mass coming from the requirement of non-erasure of the baryon asymmetry by sphalerons. After reviewing the Standard Model case we obtain this bound in two extensions…

高能物理 - 唯象学 · 物理学 2009-09-25 J. R. Espinosa

I describe a new way for baryogenesis to proceed, which evades many of the problems of GUT and electroweak scenarios. If the reheat temperature after inflation is below the electroweak scale, neither GUT baryon production nor traditional…

高能物理 - 唯象学 · 物理学 2016-11-03 Mark Trodden

The presence of a primordial magnetic field in the early universe affects the dynamic of the electroweak phase transition enhancing its strength. This effect may enlarge the window for electroweak baryogenesis in the minimal supersymmetric…

高能物理 - 唯象学 · 物理学 2009-10-31 D. Comelli , D. Grasso , M. Pietroni , A. Riotto

We discuss the possibility of generating the baryon asymmetry of the Universe when the temperature of the Universe is much below the electroweak scale. In our model the evaporation of primordial black holes or the decay of massive particles…

高能物理 - 唯象学 · 物理学 2011-05-23 Raghavan Rangarajan , Supratim Sengupta , Ajit M. Srivastava , ;

We calculate the electroweak sphaleron rates in the reduced minimal 3-3-1 (RM331) model. In the context of the early Universe, this model undergoes a sequence of two first-order phase transitions, $SU(3) \rightarrow SU(2)$ at the TeV scale…

高能物理 - 唯象学 · 物理学 2015-06-22 Vo Quoc Phong , Hoang Ngoc Long , Vo Thanh Van , Nguyen Chi Thanh

The realisation that the electroweak anomaly can induce significant baryon number violation at high temperature and that the standard models of particle physics and cosmology contain all the ingredients needed for baryogenesis has led to…

高能物理 - 唯象学 · 物理学 2009-09-25 U. A. yajnik

We describe a new mechanism for the generation of the baryon asymmetry of the universe during a first order electroweak phase transition. The mechanism requires the existence of two (or more) baryon number carrying scalar fields with masses…

高能物理 - 唯象学 · 物理学 2009-10-30 Hooman Davoudiasl , Krishna Rajagopal , Eric Westphal

We investigate whether baryogenesis is possible at a second order electroweak phase transition. We find that under rather general conditions, the departure from thermal equilibrium is suppressed by the expansion rate of the Universe, and…

高能物理 - 唯象学 · 物理学 2007-05-23 Tomislav Prokopec , Robert Brandenberger , Anne-Christine Davis

We consider the presence of cosmic string induced density fluctuations in the universe at temperatures below the electroweak phase transition temperature. Resulting temperature fluctuations can restore the electroweak symmetry locally,…

高能物理 - 唯象学 · 物理学 2009-11-07 Biswanath Layek , Soma Sanyal , Ajit M. Srivastava

For successful electroweak baryogenesis to take place through the sphaleron process the universe needs to undergo a strong first order cosmological phase transition. While it does not occur in the Standard Model it becomes possible in the…

高能物理 - 唯象学 · 物理学 2016-01-19 Anish Ghoshal
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