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GUT monopoles captured by the Sun's gravitation are expected to catalyze proton decays via the Callan-Rubakov process. In this scenario, protons, which initially decay into pions, will ultimately produce \nu_{e}, \nu_{\mu} and…

High Energy Physics - Experiment · Physics 2012-11-05 Kamiokande Collaboration , K. Ueno , K. Abe , Y. Hayato , T. Iida , K. Iyogi , J. Kameda , Y. Koshio , Y. Kozuma , M. Miura , S. Moriyama , M. Nakahata , S. Nakayama , Y. Obayashi , H. Sekiya , M. Shiozawa , Y. Suzuki , A. Takeda , Y. Takenaga , K. Ueshima , S. Yamada , T. Yokozawa , K. Martens , J. Schuemann , M. Vagins , C. Ishihara , H. Kaji , T. Kajita , K. Kaneyuki , T. McLachlan , K. Okumura , Y. Shimizu , N. Tanimoto , E. Kearns , M. Litos , J. L. Raaf , J. L. Stone , L. R. Sulak , K. Bays , W. R. Kropp , S. Mine , C. Regis , A. Renshaw , M. B. Smy , H. W. Sobel , K. S. Ganezer , J. Hill , W. E. Keig , J. S. Jang , J. Y. Kim , I. T. Lim , J. B. Albert , K. Scholberg , C. W. Walter , R. Wendell , T. Wongjirad , T. Ishizuka , S. Tasaka , J. G. Learned , S. Matsuno , T. Hasegawa , T. Ishida , T. Ishii , T. Kobayashi , T. Nakadaira , K. Nakamura , K. Nishikawa , Y. Oyama , K. Sakashita , T. Sekiguchi , T. Tsukamoto , A. T. Suzuki , Y. Takeuchi , M. Ikeda , A. Minamino , T. Nakaya , L. Labarga , Ll. Marti , Y. Fukuda , Y. Itow , G. Mitsuka , T. Tanaka , C. K. Jung , G. Lopez , I. Taylor , C. Yanagisawa , H. Ishino , A. Kibayashi , S. Mino , T. Mori , M. Sakuda , H. Toyota , Y. Kuno , M. Yoshida , S. B. Kim , B. S. Yang , H. Okazawa , Y. Choi , K. Nishijima , M. Koshiba , Y. Totsuka , M. Yokoyama , S. Chen , Y. Heng , Z. Yang , H. Zhang , D. Kielczewska , P. Mijakowski , K. Connolly , M. Dziomba , E. Thrane , R. J. Wilkes

We investigate the generation of the baryon asymmetry within the framework of cosmological gra\-vi\-ta\-tional particle production, employing the Bogoliubov approach. We examine two well-known baryogenesis scenarios, namely baryogenesis in…

High Energy Physics - Phenomenology · Physics 2024-04-11 Marcos M. Flores , Yuber F. Perez-Gonzalez

At the end of inflation the universe is frozen in a near zero-entropy state with energy density in a coherent scalar field and must be ``defrosted'' to produce the observed entropy and baryon number. We propose that the baryon asymmetry is…

High Energy Physics - Phenomenology · Physics 2009-09-29 Edward W. Kolb , Andrei Linde , Antonio Riotto

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

The interaction of a Grand Unification Magnetic Monopole with a nucleon can lead to a barion-number violating process in which the nucleon decays into a lepton and one or more mesons (catalysis of nucleon decay). In this paper we report an…

High Energy Physics - Experiment · Physics 2012-08-27 The MACRO Collaboration

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 show that a baryon asymmetry can be generated by dissipative effects during warm inflation via a supersymmetric two-stage mechanism, where the inflaton is coupled to heavy mediator fields that then decay into light species through B- and…

High Energy Physics - Phenomenology · Physics 2015-05-30 Mar Bastero-Gil , Arjun Berera , Rudnei O. Ramos , Joao G. Rosa

Magnetic monopoles are beyond standard model particles, predicted by Grand Unified Theories (GUTs) to be created during the early universe. At typical masses of the GUT-scale - above $10^{14}$ GeV - these particles would move at…

High Energy Astrophysical Phenomena · Physics 2025-07-09 Jonas Häußler , Nicolas Moller

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…

High Energy Physics - Phenomenology · Physics 2009-10-31 Lawrence M. Krauss , Mark Trodden

It has been considered that baryogenesis models without a generation of $B$-$L$ asymmetry such as the GUT baryogenesis do not work since the asymmetry is washed out by the electroweak sphalerons. Here, we point out that helical…

High Energy Physics - Phenomenology · Physics 2018-07-05 Kohei Kamada

During inflation primordial quantum fluctuations of the spacetime metric become classical and there is a spontaneous CPT violation by the spin connection coupling terms of the metric with fermions. The energy levels of the left and the…

High Energy Physics - Phenomenology · Physics 2007-05-23 Subhendra Mohanty , B. Mukhopadhyay , A. R. Prasanna

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

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 M. Plumacher

A novel mechanism, "catalyzed baryogenesis," is proposed to explain the observed baryon asymmetry in our universe. In this mechanism, the motion of a ball-like catalyst provides the necessary out-of-equilibrium condition, its outer wall has…

High Energy Physics - Phenomenology · Physics 2021-11-03 Yang Bai , Joshua Berger , Mrunal Korwar , Nicholas Orlofsky

The minimal flipped $SU(5)$ unification with the right-handed neutrino Majorana mass scale generated as a two-loop effect is arguably one of the most constrained models of perturbative baryon and lepton number violation currently on the…

High Energy Physics - Phenomenology · Physics 2025-07-01 Michal Malinský , Renato Fonseca , Václav Miřátský , Martin Zdráhal

In this review article, we revisit the topic of baryogenesis, which is the physical process that generated the observed baryon asymmetry during the first stages of the primordial Universe. A viable theoretical explanation to understand and…

General Relativity and Quantum Cosmology · Physics 2023-12-22 David S. Pereira , João Ferraz , Francisco S. N. Lobo , José P. Mimoso

We show that the baryon asymmetry produced by the out of equilibrium decay of heavy $GUT$ scalars can be the baryon asymmetry that is observed today. No restrictions need be imposed on the initial values of $B$, $L$ and $B-L$, nor on the…

High Energy Physics - Phenomenology · Physics 2014-11-17 Subir Mohan

We propose a new mechanism for baryogenesis in supersymmetric extensions of the standard model, that does not depend on (super)GUT interactions. It occurs by the non-perturbative electroweak reprocessing of a lepton asymmetry. This lepton…

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

Baryogenesis, through the decays of heavy bosons, was considered to be one of the major successes of the grand unified theories (GUTs). It was then realized that the sphaleron processes erased any baryon asymmetry from the GUT-baryogenesis…

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

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
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