1998
DOI: 10.1007/s100529800829
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Hard exclusive meson production and nonforward parton distributions

Abstract: We present an analysis of twist-2, leading order QCD amplitudes for hard exclusive leptoproduction of mesons in terms of double/nonforward parton distribution functions. After reviewing some general features of nonforward nucleon matrix elements of twist-2 QCD string operators, we propose a phenomenological model for quark and gluon nonforward distribution functions. The corresponding QCD evolution equations are solved in the leading logarithmic approximation for flavor nonsinglet distributions. We derive expl… Show more

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Cited by 124 publications
(222 citation statements)
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References 27 publications
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“…The evolution of skewed parton distributions was studied numerically in refs. [15,16,12,14,17]. In this section, we perform the numerical evolution of SPDs using the algorithm described in the previous session and present the results illustrating evolution patterns for SPDs constructed using the factorized model (3.1) with different choices for the profile function h(x, α).…”
Section: Evolution Of Nonforward Quark Distributionsmentioning
confidence: 99%
“…The evolution of skewed parton distributions was studied numerically in refs. [15,16,12,14,17]. In this section, we perform the numerical evolution of SPDs using the algorithm described in the previous session and present the results illustrating evolution patterns for SPDs constructed using the factorized model (3.1) with different choices for the profile function h(x, α).…”
Section: Evolution Of Nonforward Quark Distributionsmentioning
confidence: 99%
“…(4.23, 4.24) the momentum dependence of the constituent quark mass, M (p 2 ) cuts the loop momentum p and thus regularizes the UV divergence. Let us note that expressions (4.23, 4.24) are explicitly symmetric under transformation ξ → −ξ what follows from charge conjugation symmetry[6,5].…”
mentioning
confidence: 99%
“…For instance, the double distributions (DD) defined above have to satisfy a symmetry constraint based on hermiticity. This demands that these must be symmetric with respect to the exchange y ←→ 1 − x − y, and a profile function which respects this symmetry constraint is given by [26] π(x, y) = 6y(1 − x − y) (1 − x) 3 . (6.11)…”
Section: Jhep02(2005)038mentioning
confidence: 99%