include stdio.h #include math.h double fdet ( float d, float c, int n ); int fau ( float d, float c, int n, double ua[] ); void fld ( float d, float c, int n, double ld[] ); void fv ( int n, double vld [] ); void main() { int i, i1, j, j1, n = 5 ; float d = 2., c = 1., det ; double ld[ 10 ], ua[100], vld [100]; ...
Proton and kaon timelike form factors from Babar Sergey Serednyakov (on behalf of Babar Collaboration) Novosibirsk State University Budker Institute of Nuclear Physics, Novosibirsk The XXII International Workshop High Energy Physics and Quantum Field Theory June 24 July 1, 2015 Samara, Russia 30.06.2015 QFTHEP2015 1 OUTLINE 1. ... Advantages of ISR 1. ... At E>5 GeV the kaon FF approaches to the QCD limit 30.06.2015 QFTHEP2015 25 Thank you for attention 30.06.2015 QFTHEP2015 26 ...
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Ссылки http://qfthep.sinp.msu.ru/talks2015/1435052353_SerednQFT15.pdf -- 1090.4 Кб -- 23.06.2015 Похожие документы
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... Surface disturbance and deformat ion are shown in the same scale. Displac the free surface is much smoother as compared bottom deformations: init ial elevat ion has amplitude and spreads over a rather wide area. bottom theory, bottom ement of with the smaller F velocity potential, H depth, vector of bottom deformation, 0 initial elevation a . ... The init ial elevation assumed to be equal to the vertical bottom deformat ion (a); calculated with use of the Laplace smoothing algorithm (b). ...
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Ссылки http://ocean.phys.msu.ru/science/nosov/EGU2010_initial_condition.pdf -- 1885.8 Кб -- 12.01.2012 Похожие документы
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