Abstract
We extract the pion transverse momentum dependent (TMD) parton distribu- tion by fitting the pion-induced Drell-Yan process within the framework of TMD factoriza- tion. The analysis is done at the next-to-next-to-leading order (NNLO) with proton TMD distribution and non-perturbative TMD evolution extracted earlier in the global fit. We observe the significant difference in the normalization of transverse momentum differential cross-section measured by E615 experiment and the theory prediction.
Highlights
The numerical part of the work has been done by artemide package [17, 18]
The pion transverse momentum dependent parton distribution function (TMDPDF) obtained in this work together with distribution of 100 replicas is available in the artemide-repository [17, 18] as Vpion19 TMDPDF set
The pion-induced Drell-Yan process has been studied, with the main aim to extract the values of pion unpolarized transverse momentum dependent parton distribution function (TMDPDF)
Summary
The derivation of the cross-section for Drell-Yan process in the TMD factorization has been a subject of many studies, see e.g. refs. [5,6,7, 16]. The non-perturbative expression for DNP has been extracted in [1] together with proton TMDPDF The deviation of ζNP from its exact values at large-b could be seen as a part of non-perturbative model It adds an undesired correlation between TMDPDFs and DNP at large-b. [1] was the absence of a way to find exact ζNP at large b, where the saddle point runs to μ < ΛQCD region This problem has been solved recently by using the DNP as an independent variable that accumulates all non-perturbative information and b-dependence. In this case, expression for exact ζNP can be found order-by-order in as which is the only parameter. The computation is done at complete NNLO perturbative accuracy
Talk to us
Join us for a 30 min session where you can share your feedback and ask us any queries you have