Finite Subtractions for Meson Electroproduction and Exclusive Drell-Yan O.V. Teryaev, I.R. Gabdrakhmanov Bogoliubov Laboratory of Theoretical Physics,

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Presentation transcript:

Finite Subtractions for Meson Electroproduction and Exclusive Drell-Yan O.V. Teryaev, I.R. Gabdrakhmanov Bogoliubov Laboratory of Theoretical Physics, Joint Institute for Nuclear Research Drell-Yan Scattering and the Structure of Hadrons – Trento – May 2012

Outline Introduction: factorization, GPD, DD Relation between GPD and DD Holographic sum rule Radon transform LO photon GPD investigation Qualitative analysis of model corrections to ρ° cross section.

Factorization in perturbative QCD

Collinear GPDs

Relation between GPD and DD

Forms of Double Distributions

D-term M. V. Polyakov and C. Weiss, Phys.Rev. D60, (1999) What means: Which is particular case for:

Holographic sum rule The crucial part of DVCS and proton GPD part of the meson electroproduction O. Teryaev, arXiv:hep-ph/ (2005). I. Anikin and O. Teryaev, Phys.Rev. D76, (2007)

Radon transform

O.V. Teryaev. Crossing and Radon tomography for generalized parton distributions. Phys.\ Lett.\ B {\bf 510} (2001) 125 [

Generalized Distribution Amplitudes *O.V.Teryaev. Crossing and Radon tomography for generalized parton distributions,'' Phys.\ Lett.\ B {\bf 510} (2001) 125 [ Expression of GPD in the unphysical region |ξ |>1 via GDA was derived in the paper below

Photon GPDs

Photon GDAs

Extension of photon GPD

Holographic sum rule applied to photon GPD

Deriving photon Double Distribution D-term can be obtained from GDA:

Gauge transformations of DD Double distributions defined through Fourier image of matrix element. So one can make integration by parts and obtain

Gauge transformations of photon DD

ρ° meson electroproduction Exclusive ρ° meson electroproductionDrell-Yann ρ° p scattering

GK GPD parametrization S.V. Goloskokov, Nucl.Phys.Proc.Suppl (2011) S.V. Goloskokov, P. Kroll, Euro. Phys. J. C50, (2007) S.V. Goloskokov, P. Kroll, Euro. Phys. J. C53, (2008) GPDs are constructed from standard DD anzatz:

GK GPD parametrization S.V. Goloskokov, Nucl.Phys.Proc.Suppl (2011) S.V. Goloskokov, P. Kroll, Euro. Phys. J. C50, (2007) S.V. Goloskokov, P. Kroll, Euro. Phys. J. C53, (2008)

Subtraction corrections M. Guidal, S. Morrow.arXiv: [hep-ph] (Morrow, S.A. et al.) Eur.Phys.J. A39 (2009) arXiv: [hep-ex] Guidal-Morrow generalization of the D-term: Standard form D-term with the use of the results of the chiral quark-soliton model : M. V. Polyakov and C. Weiss, Phys. Rev. D 60, (1999) V. Y. Petrov, P. V. Pobylitsa, M. V. Polyakov, I. Bornig, K. Goeke and C. Weiss, Phys. Rev. D 57, 4325 (1998) For Nf=5 gives constant subtraction : Where :

(Morrow, S.A. et al.) Eur.Phys.J. A39 (2009) arXiv: [hep-ex] Guidal-Morrow corrections on VGG model

Qualitative estimations on d-term like corrections on GK model In assumption of small kT dependence of cross sections ratio:

Subtraction corrections Solid black – original GK Solid red – GK with CQM D-term subtraction Dashed blue – GK with Guidal –Morrow D-term CORNEL CLAS HERMES E665 ZEUS H1

Summary: Photon GPDs was extended to the full definition area Holographic sum rule was checked for photon GPD, subtraction constants were derived Photon DDs was derived using inverse Radon transform Preliminary assumptions were made for longitudinal ρ° electroproduction cross section for GK GPD model D-term like contributions can explain cross section grow at low W (further calculations are needed)