2015
DOI: 10.1142/s0217751x15500104
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Generalized Parton Distributions of proton for nonzero skewness in transverse and longitudinal position spaces

Abstract: We investigate the Generalized Parton Distributions (GPDs) of proton by expressing them in terms of overlaps of light front wave functions (LFWFs) using a simulated model which is able to qualitatively improve the convergence near the end points of x. We study the spin non-flip H(x, ζ, t) and spin flip E(x, ζ, t) part of GPDs for the particle conserving n → n overlap in the DGLAP region (ζ < x < 1). The Fourier transform (FT) of the GPDs w.r.t. to the transverse momentum transfer as well the FT of the GPDs w.r… Show more

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Cited by 14 publications
(13 citation statements)
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“…E T being an odd function of ζ, does not contribute at ζ = 0. For nonzero skewness one can also represent the GPDs in the longitudinal position space by taking FT of the GPDs with respect to ζ [9][10][11][12][13][14].…”
Section: Introductionmentioning
confidence: 99%
“…E T being an odd function of ζ, does not contribute at ζ = 0. For nonzero skewness one can also represent the GPDs in the longitudinal position space by taking FT of the GPDs with respect to ζ [9][10][11][12][13][14].…”
Section: Introductionmentioning
confidence: 99%
“…[55] using the lowest-order perturbation theory. Many other observables of the electron, e.g., the electromagnetic and gravitational form factors as well as spin and orbital angular momentum [56], generalized parton distributions (GPDs) [57][58][59][60],Wigner distributions [61], etc. have been investigated in a model based on the quantum fluctuations of the electron in QED.…”
Section: Introductionmentioning
confidence: 99%
“…We represent the spin-1 2 composite system with a mass M consist of spin- 1 2 fermion (electron) and spin-1 vector boson (photon) with respective masses m and λ. This model is also act as a guideline to nucleon strcture because electron-photon component of the physical electron can be used as a component of the nucleon wave function consists of a quark and a vector diquark and therefore it probes the structure of nucleon and widely used for the calculations of gravitational form factors and spin and orbital angualr momentum of a composite relativistic system [41], GPDs [42,43], ipdpdfs [44], charge and magnetization densities [45]. Recently this approach has been used to understand the electron TMDs in momentum plane [46].…”
Section: Introductionmentioning
confidence: 99%