... H L Z - ; 12 12 2 2 2 ew = 1+ 5 0 4 0 ln 2 M2 Z 1+ 0 0 = 0.0337; a = cos W (); 1 - a = = e ( MZ ) = ( M Z ) = 0 .0 0 7 7 5 6 ... We use values for physical masses MW = 80.4G eV , M Z = 9 1 .2 G e V , M H = 1 2 5 .1 G e V . ...
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Ссылки http://qfthep.sinp.msu.ru/proceedings2015/Plenary_Arbuzov.pdf -- 450.9 Кб -- 06.11.2015 Похожие документы
... Sk area, where k strings are overlapping, 0 single string transverse area, 0 and p0 mean multiplicity and transverse momentum from one string [5 [6 [7 [8 pt ] ] ] ] Braun, M.A. and Pajares, C. Eur. ...
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Ссылки http://qfthep.sinp.msu.ru/talks2013/V._Kovalenko__Saint_Petersburg_State_University_.pdf -- 1513.7 Кб -- 28.06.2013 Похожие документы
... m/g 2 RST conjecture: F (E ) universal Does not depend on details of the instate Checks of universality: 2 ^^^ Field theor y P (E , N ) = i ,f i |PE PN S |f Tinyakov, 1991 Projectors N N 1 Mueller, 1992 2 semiclassical instates Toy QM models Bonini et ...
... Dh don't couple with fermions. h The S field is realized as physical fields SH , SA, S‘ with masses 2 = RІ2 - І1 , M 2 = M 2 - v 2 , M 2 = M 2 - v 2 4 + 5 . ...
... 5 (or in its modification) S. Lin, E. Shuryak, 1011.1918[hep-th] I. Y. Aref'eva, A. A. Bagrov and E. O. Pozdeeva, Holographic phase diagram of quark-gluon plasma formed in heavy-ions collisions," JHEP 1205, 117 (2012) The Einstein equation for particle in ...