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Related papers: Baryogenesis at the Electroweak Scale

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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

In this lecture first I present a brief genesis of the ideas on the electroweak baryogenesis and then I focus on a mechanism in which the source of $CP$ violation is a $CP$-violating field condensate which could occur, for example, in…

High Energy Physics - Phenomenology · Physics 2007-05-23 Tomislav Prokopec

In the scenario of cold electroweak baryogenesis, oscillations of the Higgs field lead to metastable domains of unbroken phase where the Higgs field nearly vanishes. Those domains have also been identified with the $W-t-\bar{t}$ bags, a…

High Energy Physics - Phenomenology · Physics 2013-05-29 Yannis Burnier , Edward Shuryak

The presently observed cosmological baryon asymmetry has been finally determined at the time of the electroweak phase transition, when baryon and lepton number violating interactions fell out of thermal equilibrium. We discuss the…

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

We discuss electroweak baryogenesis in aligned two Higgs doublet models. It is known that in this model the severe constraint from the experimental results for the electron electric dipole moment can be avoided by destructive interference…

High Energy Physics - Phenomenology · Physics 2022-09-21 Kazuki Enomoto , Shinya Kanemura , Yushi Mura

Effect of the electroweak non-conservation of the baryon number could be a key ingredient to explain the ratio of dark and baryonic densities. If dark matter is explained by dark atoms, in which stable -2n charged particles are bound with n…

High Energy Physics - Phenomenology · Physics 2024-01-15 V. A. Beylin , M. Yu. Khlopov , D. O. Sopin

The physics of electroweak baryogenesis is described with the aim of making the essentials clear to non-experts. Several models for the source of the necessary CP violation are discussed: CKM phases as in the minimal standard model, general…

High Energy Physics - Phenomenology · Physics 2010-11-01 Glennys Farrar

Baryon asymmetry of the Universe is evaluated in the model originally proposed in Phys. Rev. Lett. 102 (2009) 051805, where Majorana masses of neutrinos are generated via three-loop diagrams composed of additional scalar bosons including…

High Energy Physics - Phenomenology · Physics 2023-06-19 Mayumi Aoki , Kazuki Enomoto , Shinya Kanemura

We demonstrate the viability of electroweak baryogenesis scenarios in which the necessary departure from equilibrium is realized by the evolution of a network of topological defects. We consider several effective models of TeV physics, each…

High Energy Physics - Phenomenology · Physics 2010-11-01 M. Trodden , A-C. Davis , R. Brandenberger

We calculate the baryon asymmetry produced at the electroweak phase transition by quasi-degenerate third generation sfermions in the minimal supersymmetric extension of the Standard Model. We evaluate constraints from Higgs searches, from…

High Energy Physics - Phenomenology · Physics 2013-05-30 Jonathan Kozaczuk , Stefano Profumo , Michael J. Ramsey-Musolf , Carroll L. Wainwright

In this talk we review the actual situation concerning electroweak phase transition and baryogenesis in the minimal supersymmetric extension of the Standard Model. A strong enough phase transition requires light Higgs and stop eigenstates.…

High Energy Physics - Phenomenology · Physics 2014-11-17 Mariano Quiros

I describe work done in collaboration with M. Joyce and K. Kainulainen on (1) the strength of the electroweak phase transition in the MSSM and (2) the mechanism for producing the baryon asymmetry during the phase transition. In the former…

High Energy Physics - Phenomenology · Physics 2007-05-23 J. M. Cline

Adding an extra singlet scalar $S$ to the Higgs sector can provide a barrier at tree level between a false vacuum with restored electroweak symmetry and the true one. This has been demonstrated to readily give a strong phase transition as…

High Energy Physics - Phenomenology · Physics 2017-06-14 James M. Cline , Kimmo Kainulainen , David Tucker-Smith

We first suggested a scenario in which a generic, dark chiral gauge group undergoes a first order phase transition in order to generate the observed baryon asymmetry in the universe, provide a viable dark matter candidate and explain the…

High Energy Physics - Phenomenology · Physics 2012-02-15 Devin G. E. Walker

In the electroweak phase transition there arises the problem of baryon number washout by sphaleron transitions, which can be avoided if the phase transition is strongly enough first order. The phase transition in the Standard Model or in…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. T. Davies , C. D. Froggatt , G. Jenkins , R. G. Moorhouse

We correct a numerical error which led to an overestimate of the baryon asymmetry from supersymmetric electroweak baryogenesis in our paper JHEP07(2000)018. Updated dependences of the baryon asymmetry on chargino mass parameters and the…

High Energy Physics - Phenomenology · Physics 2007-05-23 James M. Cline , Michael Joyce , Kimmo Kainulainen

The sphaleron type solution in the electroweak theory, generalized to include the dilaton field, is examined. The solutions describe both the variarions of Higgs and Gauge fields inside the sphaleron and the shape of the dilaton cloud…

High Energy Physics - Theory · Physics 2007-05-23 D. Karczewska , R. Manka

We discuss the generation of the baryon asymmetry by a strong first order electroweak phase transition in the early universe, particularly in the context of the MSSM. This requires a thorough numerical treatment of the bubble wall profile…

High Energy Physics - Phenomenology · Physics 2014-11-17 S. J. Huber , P. John , M. G. Schmidt

We present arguments that the CKM CP-violation in the standard model may be sufficient for the generation of the baryon asymmetry, if the electroweak transition in the early universe was of the cold, tachyonic, type after electroweak-scale…

High Energy Physics - Phenomenology · Physics 2017-08-23 Jan Smit

We calculate the dissipation of the baryon number after the electroweak phase transition due to thermal fluctuations above the sphaleron barrier. We consider not only the classical Boltzmann factor but also fermionic and bosonic one-loop…

High Energy Physics - Phenomenology · Physics 2009-10-28 D. Diakonov , M. Polyakov , P. Sieber , J. Schaldach , K. Goeke
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