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Leading Effects in the Spectra of L c and anti L c Produced in S - p, pp and p - p Interactions. Olga Piskounova, P.N.Lebedev Physical Institute,. Quark-Gluon String Model. N-Pomeron exchange diagram illustrates the multiparticle production at high energy. O.Piskounova.
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LeadingEffects in the Spectra ofLcandantiLcProduced inS- p, pp andp- p Interactions. Olga Piskounova, P.N.Lebedev Physical Institute,
Quark-Gluon String Model N-Pomeron exchange diagram illustrates the multiparticle production at high energy. O.Piskounova
Valence Quark Distributions in QGSM O.Piskounova Inclusive production cross section of hadrons H is written as a sum over n-Pomeron cylinder diagrams: Distribution functions of Lc in p-p collisions are given by:
Diquark Fragmentation Function and String Junction Transfer Diquark fragmentation function includes the constant afLc that can be interpreted as “leading” paremeter: where the term z2aR(0)-2aN(0) means the probability for diquark to have z close to 0. Fragmentation function of string junction is of the similar form: where aSJ(0)=0,5. O.Piskounova
D meson asymmetry in pp O.Piskounova c
Lc /antiLc asymmetry in Sp O.Piskounova
Lc /antiLc asymmetry in pp O.Piskounova
Conclusions The nonzero baryon/antibaryon asymmetry in pion reaction is sensitive to the features of baryon charge transfer by the proton string junction. This effect should be seen in muon- and photon-proton colisions The charmed baryon/antibaryon spectra were discribed with the same leading fragmentation parameter af=0.006 There is no need to involve “intrinsic charm” in the calculation of charmed baryon spectra at the up-to-date level of experimental data O.Piskounova