Abstract

We present a calculation of valence double parton distributions of the pion in the framework of chiral quark models. The result obtained at the low-energy quark model scale is particularly simple, where in the chiral limit a factorized form follows, D(x1,x2,q⃗)=δ(1−x1−x2)F(q⃗)D(x_1,x_2, \vec{q}) = δ(1-x_1-x_2) F(\vec{q}) with x1,2x_{1,2} standing for the longitudinal momentum fractions of the valence quark and antiquark, and q⃗\vec{q} denotes the relative transverse momentum. For q⃗=0⃗\vec{q}=\vec{0} the result satisfies the Gaunt-Sterling sum rules. The QCD evolution to higher scales is carried out within the dDGLAP framework. We argue that the ratios of the valence Mellin moments ⟨x1nx2m⟩/⟨x1n⟩⟨x2m⟩\langle x_1^n x_2^m \rangle / \langle x_1^n \rangle \langle x_2^m \rangle , which do not depend on the dDGLAP evolution, provide particularly convenient measures of the longitudinal correlations between the partons. Such ratios could be probed in future lattice QCD simulations.

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