... ert (q 2 ) (4) Lomonosov Moscow State University QFTHEP 2015 Introduction QCD Sum rules Numerical analysis яonclusions B m -q 2 1 2 =e -m2 T (5) Finally we apply Borel transformation (inverse Laplace transformation) to the both parts of Sum rules, which ...
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Ссылки http://qfthep.sinp.msu.ru/talks2015/Chesnokov_QFTHEP%202015.pdf -- 707.1 Кб -- 27.06.2015 Похожие документы
... SCALAR MODEL ABELIAN MODEL ANALYSIS QUANTUM CORRECTION CONCLUSION m , Ge V n 2 2 f (2330) 0 5 f (2200) 0 4 f (2020) 0 3 f (1710 ... 1 2 3 4 5 6 7 8 9 10 M 2 /M 2 0 ALISA KATANAEVA LAGRANGIAN ALTERNATIVE TO QCD STRING SPBSU. ...
... with opposite charge p >20 GeV/c ||<2.4 (muon) T p >20 GeV/c ||<2.5 (electron) T One or two jets with p >30 GeV/c and ||<2.4, at least T one jet is b-tagged MET>30 GeV Additional cuts: 2 m >20 GeV/c ll 2 2 veto events with 81 GeV/c <m < 101GeV/c ll H > 60 ...
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Ссылки http://qfthep.sinp.msu.ru/talks2013/tsirova_qfthep_2013-06-25.pdf -- 1180.3 Кб -- 25.06.2013 Похожие документы
... N. P. Zotov5 1 P. N. Lebedev Institute of Physics, 53 Lenin Avenue, 119991 Moscow, Russia 5 D. V. Skobeltsyn Institute of Nuclear Physics, M. V. Lomonosov Moscow State University, Leninskie Gory 1, 119991 Moscow, Russia 2 ,3 ,4 , Associated production of ...
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Ссылки http://qfthep.sinp.msu.ru/proceedings2015/Collider_Baranov.pdf -- 104.7 Кб -- 06.11.2015 Похожие документы
... arg( 6, 7 12 2 , 7 ) =arg( 5 )/2 One-loop (t, b)CP U eff contributions mtop at the MS USY U is CP-invariant =0 scale, because µ - massscale 4 SUSY Eff. potential method energy or Feynman diags (temperature T) M Scalar sector for MSSM The main contribution ...
... 5 2) N gauge bosons: ( N 1) vertices M N vector bosons M0 l 1 N M l M l N vertices 6 3 1 2 S (ql ) j 1 N S (k for l 1, , N 1; j l 1 3 M 0 ~ i 2 N 1 f out ( pout ) S 1 ( pout ) S 1 (k0 ) m fout 2 Ml ~ i 2 N 1 l j f out ( pout ) j S (q j ) S 1 (kl ) m fl j ...
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Ссылки http://qfthep.sinp.msu.ru/talks2015/1435268650_QFTHEP_Svirina6.pdf -- 774.0 Кб -- 25.06.2015 Похожие документы