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We develop the minimal model of a new leading order parameterization of GPDs introduced by Shuvaev and Polyakov. The model for GPDs H and E is formulated in terms of the forward quark distributions, the Gegenbauer moments of the D-term and the forward limit of the GPD E. The model is designed primarely for small and medium-size values of x_B, x_B leq 0.2. We examined two different models of the t-dependence of the GPDs: The factorized exponential model and the non-factorized Regge-motivated model. Using our model, we successfully described the DVCS cross section measured by H1 and ZEUS, the moments of the beam-spin A_{LU}^{sin phi}, beam-charge A_{C}^{cos phi} and transversely-polarized target A_{UT}^{sin phi cos phi} DVCS asymmetries measured by HERMES and A_{LU}^{sin phi} measured by CLAS. The data on A_{C}^{cos phi} prefers the Regge-motivated model of the t-dependence of the GPDs. The data on A_{UT}^{sin phi cos phi} indicates that the u and d quarks carry only a small fraction of the proton total angular momentum.
We explore the application of a two-component model of proton structure functions in the analysis of deep-inelastic scattering (DIS) data at low $Q^2$ and small $x$. This model incorporates both vector meson dominance and the correct photo-production
Initial state evolution in parton shower event generators involves parton distribution functions. We examine the probability for the system to evolve from a higher scale to a lower scale without an initial state splitting. A simple argument suggests
We correct the mistaken claim made in cite{Guzey:2005ec,Guzey:2006xi} that the minimal model of the dual parameterization of nucleon generalized parton distributions (GPDs) gives a good, essentially model-independent description of high-energy data o
In addition to the inclusive cross sections discussed within the QCD-parton model, in the regime of multiple parton interactions, different and more exclusive cross sections become experimentally viable and may be suitably measured. Indeed, in its st
The organization of finite order QCD approximations to $F_2^{gamma}(x,Q^2)$ based on the separation of pure QED contribution from those of genuine QCD nature is discussed.