2009
DOI: 10.1140/epjc/s10052-009-1073-4
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Generalized parton distributions from hadronic observables: non-zero skewness

Abstract: We propose a physically motivated parametrization for the unpolarized generalized parton distributions, H and E, valid at both zero and non-zero values of the skewness variable, ζ. Our approach follows a previous detailed study of the ζ = 0 case where H and E were determined using constraints from simultaneous fits of the experimental data on both the nucleon elastic form factors and the deep inelastic structure functions in the non singlet sector. Additional constraints at ζ = 0 are provided by lattice calcul… Show more

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Cited by 28 publications
(43 citation statements)
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References 63 publications
(167 reference statements)
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“…By inspecting Eqs. (27), (29) and (48) one can see that for t = 0 and ζ = 0, the only parameters that enter are: As already noticed in [24][25][26], the diquark model based parametrization corresponds to a low initial scale, Q 2 o . Parametric forms are then evolved to the Q 2 of the data using LO Perturbative QCD (PQCD) evolution equations [37].…”
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confidence: 74%
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“…By inspecting Eqs. (27), (29) and (48) one can see that for t = 0 and ζ = 0, the only parameters that enter are: As already noticed in [24][25][26], the diquark model based parametrization corresponds to a low initial scale, Q 2 o . Parametric forms are then evolved to the Q 2 of the data using LO Perturbative QCD (PQCD) evolution equations [37].…”
mentioning
confidence: 74%
“…The number of parameters used is consistent with the one used in fits of the nucleon form factors data. These require four parameters for G q and E q from [24,25] at the scale Q 2 o , is also shown. In Fig.7 we show H u,d (X, ζ, t; Q 2 ) evaluated at Q 2 = 2 GeV 2 and for a variety of ranges in ζ ≡ x Bj and Q 2 .…”
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confidence: 82%
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“…In this work, we investigate a recent parametrization [18] of the GPDs in position space for non-zero ζ. GPDs for zero skewness have been parametrized in a similar way in [19]. At the input scale they are parametrized by a spectator model term multiplied by a Regge motivated term.…”
Section: Introductionmentioning
confidence: 99%
“…Initial work [4] in constructing a spectator model for the chiral even GPDs, H q (X, ζ ,t) and E q (X, ζ ,t), showed considerable promise in incorporating constraints and in confronting data. This approach was extended to include all four of the chiral even valence quark GPDs, in conjunction with Deeply Virtual Compton Scattering (DVCS), in a series of papers that developed the "flexible model", which is a "Reggeized diquark model" (R x Dq) [5,6].…”
Section: Introductionmentioning
confidence: 99%