... theory is described by the potential [6] V = m 2 11 # + 1 # 1 +m 2 22 # + 2 # 2 - [m ... 2 A /v 2 # # # (7) after eliminating m 2 11 , m 2 22 , m 2I 12 from the minimization ...
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Ссылки http://theory.sinp.msu.ru/~qfthep04/2004/Proceedings2004/Kalinowski_QFTHEP04_204_211.ps -- 523.1 Кб -- 17.09.2009 Похожие документы
... Recent Results from CDF . M. Gallinaro 1 . Charm Hadroproduction Results from Selex . M. Iori 11 . The Structure of the Proton . R. Lahmann 15 . ...
... Physics Letters A 341 (2005) 467472 471 Substituting the mass (14) in the moment of inertia (11), we get the relation ( M R 2 ... 11] M. Schroeder, Fractals, Chaos, Power Laws, Freeman, New York, 1990, Section 10. [12] V.E. Tarasov, Phys. Lett. ...
... of the kth particle, Fk is the force that acts on the kth particle, and m q1 V 11 ... M. F. Shlesinger, "The wonderful world of random walks," in Studies in Statistical ... 11M. Naber, "Time fractional SchrЖdinger equation," J. Math. ...
... 2: Stop mass m t 1 (the left figure for tg# =5) and sbottom mass m b1 (the right figure for tg# =40) in the CPX scenario [11 ... B375 (1996) 203 [11] M. Carena, J. Ellis, A. Pilaftsis, C. Wagner, Phys.Lett. B495 (2000) 155 185. ...
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Ссылки http://theory.sinp.msu.ru/~qfthep04/2004/Proceedings2004/Akhmetzyanova_QFTHEP04_178_185.ps -- 1158.0 Кб -- 17.09.2009 Похожие документы