In order to learn effectively from measurements of generalised parton distributions (GPDs), it is desirable to compute them using a framework that can potentially connect empirical information with basic features of the Standard Model. We sketch an approach to such computations, based upon a rainbowladder (RL) truncation of QCD's Dyson-Schwinger equations and exemplified via the pion's valence dressed-quark GPD, H v (x, , t). Our analysis focuses primarily on = 0, although we also capitalise on the symmetry-preserving nature of the RL truncation by connecting H v (x, =1, t) with the pion's valence-quark parton distribution amplitude. We explain that the impulse-approximation used hitherto to define the pion's valence dressed-quark GPD is generally invalid owing to omission of contributions from the gluons which bind dressed-quarks into the pion. A simple correction enables us to identify a practicable improvement to the approximation for H v (x, 0, t), expressed as the Radon transform of a single amplitude. Therewith we obtain results for H v (x, 0, t) and the associated impact-parameter dependent distribution, q v (x, | b |), which provide a qualitatively sound picture of the pion's dressedquark structure at ah a d r o n i c scale. We evolve the distributions to a scale = 2G e V , so as to facilitate comparisons in future with results from experiment or other nonperturbative methods.
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Mezrag et al. (2014) studied this question.