... The hard partonic subprocess g g QQ amplitude is describ ed by three Feynman's diagrams, 20 N.P. Zotov, QFTHEP 2011 Sochi, Russia, Sep. 27, 2011 which corresp ond to m.e. p 1 - q1 + M ^ ^ ( -i g ) ( p 1 - q1 ) 2 - M 2 p 1 - q2 + M ^ ^ ( -i g µ ) µ M2 = u ...
... The measurement is done on the f S M coefficient, which express the degree of spin correlation with M respect to the Standard Model prediction, which is ASel icity = 0.318 ± 0.005, obtaining h f SM = 1.20 ± 0.05 (stat.) ± 0.13 (syst.) ...
... 2013 - 034 1.6 ± 0.3 1.5 ± 0.4 1.0 ± 0.3 0.8 ± 0.7 : -0.4 ± 1.0 M CMS-PAS-HIG-13-005, 13-012 H - : 0.77 ± 0.27 H - Z Z : 0.92 ± 0.28 H - W W : 0.68 ± 0.20 H - : 1.10 ± 0.41 V H - V bb : 1.00 ± 0.49 I am grateful to Ilya Tsukerman for proper references ...
... 50 40 Count 30 f LQCD B = 191.5 ± 7.3 MeV 20 10 0 4.1 4.2 b 4.3 4.4 m (GeV) Distribution of mb range fB = (191.5 with the associated distributions in the as obtained by the bootstrap analysis: Gaussian distributions for fB in the ± 7.3) MeV and for all ...
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Ссылки http://qfthep.sinp.msu.ru/talks2013/Talk_Melikhov_QFTHEP2013.pdf -- 240.8 Кб -- 21.06.2013 Похожие документы
... m Tm (µ) , Tq (µ) = - e2 Y ( , ). r3 q 4 XXIInd International Workshop "High-Energy Physics and Quantum Field Theory", June 24 July 1, 2015, Samara, Russia To obtain the quadrupole interaction contribution we have to calculate diagonal and off-diagonal ...
... Xumeu Planells e+e - excess from local LPB 20 Backup I Explicit formula for the simulation with acceptance correction: dN = d 4 xdM в acc. ~ dM ~ 1 (M - M ) exp - 2 2 1 kt dkt dyd pt 2 2 2 cV P 2 ~ 24 M ~ M 2g 1- V ~ M µ 2 n2 m 2 32 / ~ |Ek p - k Ep | ...
... 4 mB ) G 2 m 2 E (1 cos 2 ) (e e NN ) 4 2 C 2 3m GM 2 2 2mB G 2 m 2 E Effective form ... m < 4 GeV - LA ISR 2 - PhysRevD.88.072009(2013), m =3 6 GeV - SA ISR 30.06.2015 ... S (m ) C ~422 m4 m ln ( m / 2 2 ) FF ~ 1 at threshold N(1520)N(1520)? ...
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Ссылки http://qfthep.sinp.msu.ru/talks2015/1435052353_SerednQFT15.pdf -- 1090.4 Кб -- 23.06.2015 Похожие документы