... we get the formal equality of the functional integrals 11 2 exp - ((t)) dt d = 2 0 t ... in the exponent is the well-known Ito stochastic integral t=1 t=0 1 13 3 (1) - (0 ...
... 4 r where we do not write the integral for the one-loop ghost contribution and the integrals I0 I4 are given below, and the following notation is used: tr (T A T B ) T (R) f AC D B C D AB $ ; (T A )i k (T A )k j C (R)i j ; r AA . ...
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Ссылки http://nuclphys.sinp.msu.ru/conf/lpp14/220809/Stepanyantz.pdf -- 469.9 Кб -- 16.09.2009 Похожие документы
... 7 NEW INTEGRAL REPRESENTATION FOR D(Q2) This ob jective can b e achieved by deriving the integral representations for the Adler function and R(s)-ratio, which involve a common sp ectral function. ...
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Ссылки http://nuclphys.sinp.msu.ru/conf/lpp14/210809/nesterenko.pdf -- 222.6 Кб -- 16.09.2009 Похожие документы
... det D2)-2dµ (10) Here the measure dµ includes the gauge fixing factor and FaddeevPop ov ghosts and the measure dµ includes also differentials of the ~ fields , , b, e. The integral reduces to the usual path integral for ~ the Yang-Mills scattering matrix ...
... Moscow, 2013) 6 ћ The obtained integral representations automatically emb o dy all ... In the massless limit (m = 0) integral representations read q2 1 - ( /q 2) d ...
... 18 10 19 10 20 10 21 E, eV GZK CUTOFF IN HiRes INTEGRAL SPECTRUM 1.2 1 J(>E)/KE - 0.8 0.6 0.4 0.2 0 17 17.5 18 18.5 19 19.5 20 20.5 21 log10(E) (eV) E1/2 in HiRes integral spectrum confirms that steepening in the differential spectrum is the GZK cutoff: E ...
... DM models Numerical simulations 3 kp c N = 62 106 , m = 1 .2 1 0 -10 60 p c M , 0.024 pc z = 350 26 (Diemand, Moore, Stadel, 2005) Integral mass function and numb er density of clumps dM dM 0.02(n + 3) M M (r ) DM ncl (M , R )d ln Md ln R = (M , )d ln Md ...
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Ссылки http://nuclphys.sinp.msu.ru/conf/lpp14/210809/Berezinsky_Dokuch_Erosh.pdf -- 233.2 Кб -- 16.09.2009 Похожие документы
... in 3-loop NNLO : · Analytic regularization of the kinematic factor / M.Nekrasov,2007 / analytic calculation of "singular" integrals · Conventional-perturbation-theory definition of the "test" function Model for testing MPT : · · Test function : tree-level ...
... A0 (z ) = dz a n 2 kn constant zero mode - overlap integral is finite Kirpichnikov Dmitriy Quasilocalization in high-energy collisions Charge universality S i nt = d 4x dz a 2 kn 4+ n e5 A0 (z ) 0 (z ) 0 (z ) (x ) µ (x ) Aµ (x ) e5 = e S = 5 - dimensional ...
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Ссылки http://nuclphys.sinp.msu.ru/conf/lpp14/220809/Kirpichnikov.pdf -- 72.1 Кб -- 16.09.2009 Похожие документы