... by the symmetry: L= f п[ 2 m MR І ], [ І ][ ] R 5 N , ; V. Shklyar, H. Lenske, Phys ... 0 .5 0 .0 - 0 .5 - 1 .0 0 p N (1 5 2 0 ) 0 .4 0 .2 F 2 M A ID 2 0 0 7 JL a b -M S U ...
... d xe |T j5( x) (0) |, i px ( j 5 j5( x) = (mQ + m)qi5 Q( x) п Physical QCD vacuum ... s), s, ) (mb, s, ) (mb, s, s) To 2 -accuracy, m s i i s 5 4 Pole mass OPE 3 2 1 0 i ...
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Ссылки http://qfthep.sinp.msu.ru/talks2011/Melikhov_QFTHEP2011.pdf -- 578.8 Кб -- 05.10.2011 Похожие документы
... QCD boundar y of a strong interaction (non-perturbative region) is around 600 M eV where s 0.5 that is coupling gs = 4 s = 2.5 ... B, 656, 67 (2007). [5] B.A. Arbuzov, M.K. Volkov and I.V. Zaitsev, Int. Journ. Mod. Phys. A 24, 2415 (2009). ...
... uncertainty EPA = nominal 4.07 pb CMS (m +- +- , 40 pb-1 T > 11.5 GeV, p > 4 GeV ... 3 in c l. WW 3.5 [fb] 26 June 2015 M. Dyndal (on behalf of the ATLAS Collaboration ...
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Ссылки http://qfthep.sinp.msu.ru/talks2015/1435295464_mdyndal_2015-06-26_QFTHEP15.pdf -- 2852.2 Кб -- 26.06.2015 Похожие документы
... k ) L D k 1 2 -2 k 2 µ - k µ · k ptil g vetorF µ = (H, -x , H, H) X dispersion lws k1 k1± = L= k10 = 2 - - m 2 - 2 k 2 k 28.06.13 5 / 19 2 - m 2 k 2 x 2 - S. Kolevatov (SPbSU) ^ k = ( , ^ k2 , k3 ), x = (x0 , ^^ x2 , x3 ) : k · x = - x0 + k2 x2 + k3 x3 ...