|
چکیده
|
The next-to-leading order (NLO) unintegrated parton distribution functions (UPDF) are calculated in the two schemes by using the latest version of the integrated parton distribution functions (PDF) ofMartin et al. (MSTW2008) as the inputs and the final results are compared among each others. In the first method, socalled the Kimber–Martin–Ryskin (KMR) prescription, the Dokshitzer–Gribov–Lipatov–Altarelli–Parisi (DGLAP) collinear approximation is used, instead of the Ciafaloni–Catani–Fiorani–Marchesini (CCFM) evolution equations and the dependence of PDF on the second scale, kt (the partons transverse momenta), beside the first scale, μ (μ is the probe scale), is included in the last step of DGLAP evolution equation. In the second approach, which has been proposed by Martin, Ryskin and Watt (MRW), the current scale, the splitting functions, etc are modified in the KMR procedure. The three-dimensional UPDF are presented in terms of different [x, k2 t ]-planes for the large values of x (the longitudinal fraction of parton momentum) at μ2 = 102 and 104 GeV2. It is shown that as in MRW calculations, at each μ2 a kink is observed around k2 t μ2 and k2 t 0.38μ2 for the KMR and the MRW formalisms, respectively. Finally, it is demonstrated that the MRW gluon UPDF decrease with respect to the KMR ones, except of the small k2 t regions, i.e. the Higgs production domain, so it can be concluded that the application of the MRW procedure may improve the exclusive reaction cross sections.
|