K. M. Belotsky
National Research Nuclear University MEPhI
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Featured researches published by K. M. Belotsky.
Physical Review D | 2003
K. M. Belotsky; Daniele Fargion; M. Khlopov; Rostislav Konoplich; K. Shibaev
Results from several recent experiments provide inderect evidences in the favor of existence of a 4th generation neutrino. Such a neutrino of mass about 50 GeV is compatible with current physical and astrophysical constraints and well motivated in the framework of superstring phenomenology. If sufficiently stable the existence of such a neutrino leads to the drastic change of Higgs boson physics: for a wide range of Higgs boson masses the dominant mode of Higgs boson decay is invisible and the branching ratios for the most promising modes of Higgs boson search are significantly reduced. The proper strategy of Higgs boson searches in such a framework is discussed. It is shown that in the same framework the absence of a signal in the search for invisible Higgs boson decay at LEP means either that the mass of Higgs is greater than 113.5 GeV or that the mass difference between the Higgs mass and doubled neutrino mass is small.
Physics of Atomic Nuclei | 2008
K. M. Belotsky; Daniele Fargion; M.Yu. Khlopov; Rostislav Konoplich
Primordial heavy neutrinos of the fourth generation might explain different astrophysical puzzles. The simplest fourth-neutrino scenario is consistent with known fourth-neutrino physics, cosmic ray antimatter, cosmic gamma fluxes, and positive signals in underground detectors for a very narrow neutrino mass window (46–47 GeV). However, accounting for the constraint of underground experiment CDMS prohibits solution of cosmic-ray puzzles in this scenario. We have analyzed extended heavy-neutrino models related to the clumpiness of neutrino density, new interactions in heavy-neutrino annihilation, neutrino asymmetry, and neutrino decay. We found that, in these models, the cosmic-ray imprint may fit the positive underground signals in DAMA/Nal experiment in the entire mass range 46–70 GeV allowed from uncertainties of electroweak parameters, while satisfaction of the CDMS constraint reduces the mass range to around 50 GeV, where all data can come to consent in the framework of the considered hypothesis.
arXiv: Astrophysics | 2006
K. M. Belotsky; K. I. Shibaev
Stable neutrino and U quark of 4th generation are excluded neither by experimental data, nor by astrophysical constraints. Moreover, excess of stable
Modern Physics Letters A | 2014
K. M. Belotsky; A. D. Dmitriev; E. A. Esipova; V. A. Gani; A. V. Grobov; M. Yu. Khlopov; A. A. Kirillov; S. G. Rubin; I. V. Svadkovsky
\bar U
Advances in High Energy Physics | 2014
K. M. Belotsky; Maxim Yu. Khlopov; Chris Kouvaris; Maxim Laletin
quarks in the Universe can lead to an exciting composite nuclear-interacting form of dark matter, which can even dominate in large scale structure formation.Stable neutrino and U quark of 4th generation are excluded neither by experimental data, nor by astrophysical constraints. Moreover, excess of stable
Physical Review D | 2009
K. M. Belotsky; Maxim Yu. Khlopov; Chris Kouvaris
\bar U
Gravitation & Cosmology | 2011
K. M. Belotsky; A. V. Berkov; A. A. Kirillov; S. G. Rubin
quarks in the Universe can lead to an exciting composite nuclear-interacting form of dark matter, which can even dominate in large scale structure formation.
Physics of Atomic Nuclei | 2002
K. M. Belotsky; M. Yu. Khlopov; K. I. Shibaev
The nonbaryonic dark matter of the Universe is assumed to consist of new stable forms of matter. Their stability reflects symmetry of micro world and mechanisms of its symmetry breaking. In the early Universe heavy metastable particles can dominate, leaving primordial black holes (PBHs) after their decay, as well as the structure of particle symmetry breaking gives rise to cosmological phase transitions, from which massive black holes and/or their clusters can originate. PBHs can be formed in such transitions within a narrow interval of masses about
Journal of Cosmology and Astroparticle Physics | 2017
K. M. Belotsky; Ruslan Budaev; A. A. Kirillov; Maxim Laletin
10^{17}
Physics of Atomic Nuclei | 2000
K. M. Belotsky; Yu. A. Golubkov; M. Yu. Khlopov; R.V. Konoplich; Alexander Sakharov
g and, avoiding severe observational constraints on PBHs, can be a candidate for the dominant form of dark matter. PBHs in this range of mass can give solution of the problem of reionization in the Universe at the redshift