Minimal model of the dual parameterization of nucleon GPDs

V. Guzey and T. Teckentrup, Phys. Rev. D 74, 054027 (2006)
V. Guzey and T. Teckentrup, Phys. Rev. D. 79 , 017501 (2009) [arXiv:0810.3899 [hep-ph]]


Description of the model

Comparison to DVCS data

Compton Form Factors
of proton and neutron
(with downloads)

DVCS asymmetries
ALU, AC and AUT
of proton and neutron
(with downloads)

Nuclear GPDs and nuclear
DVCS asymmetries (with downloads)







Back to V.Guzey at PNPI

Compton Form Factors

The so-called Compton Form Factors (CFFs) are defined as convolution of GPDs with the leading-order hard scattering coefficients:

dual_cffs_f1
Note that the CFFs defined above differ by an overal minus sign from the CFFs of BMK (A.V. Belitsky, D. Mueller and A. Kirchner, Nucl. Phys. B629 (2002) 323)

Dual parameterization predictions for the proton and neutron CFFs

Using the dual parameterization of nucleon GPDs, we calculated the proton and neutron CFFs for the GPDs H and E as a function of all three variables xB, Q2 and t in the following kinematic range, 0.01 < xB < 0.5, 1 < Q2 < 10 GeV2 and 0.005 < |t| < 1 GeV2, and for a wide range of Ju and Jd, -0.6 < Ju < 0.6 and -1 < Jd < 1.
The generated CFFs are given as 3D grids.

Those grids and the interpolating routines in Fortran, which enable the user to obtain the CFFs at the desired values of xB, Q2, t, Ju and Jd can be downloaded following the links below.

Proton Neutron
Grid for the proton CFF H
Grids for the proton CFF E
Interpolating routine for the proton CFFs H and E
Grid for the neutron CFF H
Grids for the neutron CFF E
Interpolating routine for the neutron CFFs H and E