... Студеникин Александр Иванович (20.03.1957). ... Создал и читает курсы лекций 'Электрослабые процессы в сильных электромагнитных полях', 'Взаимодействие элементарных частиц в электромагнитных полях' и 'Введение в физику нейтрино'. ... Neutrino and electrons in background matter: a new approach', Annales de la Fondation Louis de Broglie 31 (2006) ? ... Quantum treatment of neutrino in background matter', J. Phys. A: Math. ... Neutrino quantum states and spin light in matter' (with A.Ternov), Phys....

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• Казаков Кирилл Александрович
• Kirill A. Kazakov

Cosmic Research, Vol. 42, No. 5, 2004, pp. 435­488. Translated from Kosmicheskie Issledovaniya, Vol. 42, No. 5, 2004, pp. 453­508. Original Russian Text Copyright © 2004 by Veselovsky, Panasyuk, Avdyushin, Bazilevskaya, Belov, Bogachev, Bogod, Bogomolov, Bothmer, Boyarchuk, Vashenyuk, Vlasov, Gnezdilov, Gorgutsa, Grechnev, Denisov, Dmitriev, Dryer, Yermolaev, Eroshenko, Zherebtsov, Zhitnik, Zhukov, Zastenker, Zelenyi, Zeldovich, Ivanov-Kholodnyi, Ignat'ev, Ishkov, Kolomiytsev, Krasheninnikov, Kudela,

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• http://www.kosmofizika.ru/buri/pansyketal.pdf

... L Сd , Pol a nd ABOUT EFFECTIVE MODES METHOD FOR DESCRIPTION OF INTERNAL DYNAMICS OF WEAKLY BOUND CLUSTERS Elena Belega, Evgeny Cheremukhin 1 , Dmitry Trubnikov Abstract: New approach to describe the internal dynamics of weakly bound clusters is presented. ... It is found that the number of active collective modes depends on the initial cluster excitation and that the internal energy is partitioned nonuniformly among the modes. ... Collective motion of oxygen atoms performs mostly in plane. ...

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• http://beams.chem.msu.ru/sotrudniki/larin/IJQCh_04.pdf
• http://beams.chem.msu.ru/sotrudniki/larin/PCCP1.pdf
• Белега Елена Дмитриевна - Лаборатория молекулярных пучков МГУ

... Formulation of the problem ­ angle about the mass center C IC = mR 2 ­ central moment of inertia m and R ­ mass and radius of the hula-hoop k ­ coefficient of viscous friction r ­ radius of the waist FT ­ friction force N ­ reaction force ­ angle between x and CO x = a sin t , IC m m Ё +k (R - (R - y = b cos t = -FT R r ) = m (x sin + y cos ) + FT Ё Ё Ё r ) 2 = m (x cos - y sin ) + N Ё Ё (R - r ) = R ­ non-slippage where constants 0 mod 2 are defined from + µ cos 0 = 0. ...

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• Anton O. Belyakov

... Consider a matrix S. The element sij of S is equal to the number of inextendible directed sequences from the minimal vertex i to the maximal vertex j . ... Therefore the number of directed sequences from the vertex i to the vertex j is equal to the element wij of a matrix W: N W= k =0 V k , (1 9 ) 6 where N is equal to the number of edges in the graph. ... Tr S is equal to the number of inextendible directed sequences from minimal vertexes to maximal vertexes that have equal numbers. ...

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• http://temporology.bio.msu.ru/EREPORTS/korotaev_experimental.pdf
• http://temporology.bio.msu.ru/EREPORTS/krugly_discrete.pdf
• http://temporology.bio.msu.ru/EREPORTS/krugly_discrete-sequential.pdf

Contents Curricula, and Programs. Mathematical Analysis. (The Program of Mathematical Physics Department).............................................. Algebra and Analytical Geometry.(The program of (General "Mathematics" Department)................................ Computer and Programming. (The program of Algorithmic Languages Department).................................... The practical work on Computers.( Department of Algorithmic. Languages)............................................... Discrete

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Introduction to PLASMA ASTROPHYSICS (Selected 10 lectures) Boris V. Somov Astronomical Institute and Faculty of Physics Moscow State University Pushino-na-Oke, 2008 Contents Ab out These Lectures 1 Particles and Fields: Exact Self-Consistent Description 1.1 Liouville's theorem . . . . . . . . . . . . . . . . . . . 1.1.1 Continuity in phase space . . . . . . . . . 1.1.2 The character of particle interactions 1.1.3 The Lorentz force, gravity . . . . . . . . . 1.1.4 Collisional friction . . . . . . . . . . . .

228. InCo literature in English

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