Wave Functions, Evolution Equations and Evolution Kernels from Light-Ray Operators of QCD

D. Müller, D. Robaschik, B. Geyer, F.-M. Dittes, J. Hořejší

Fortschritte der Physik/Progress of Physics · 1994 · 1.2K citations · 26 references

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TL;DR

QCD wave functions and distribution functions are defined as matrix elements of light‑ray operators, which arise as the large‑momentum limit of non‑local hadron operators or as sums of local operators in light‑cone expansions. The authors derive evolution equations and kernels for these two‑variable distribution amplitudes from the renormalization‑group equation of the light‑ray operators, using the analytic properties of their anomalous dimensions obtained via the α‑representation of Green’s functions. They introduce non‑forward one‑particle matrix elements that generate new distribution amplitudes describing two hadrons simultaneously, apply them to exclusive virtual Compton scattering and two‑meson production, and confirm relations between Altarelli–Parisi and Brodsky–Lepage kernels against two‑loop QCD calculations.

Abstract

The widely used nonperturbative wave functions and distribution functions of QCD are determined as matrix elements of light-ray operators. These operators appear as large momentum limit of non-local hadron operators or as summed up local operators in light-cone expansions. Nonforward one-particle matrix elements of such operators lead to new distribution amplitudes describing both hadrons simultaneously. These distribution functions depend besides other variables on two scaling variables. They are applied for the description of exclusive virtual Compton scattering in the Bjorken region near forward direction and the two meson production process. The evolution equations for these distribution amplitudes are derived on the basis of the renormalization group equation of the considered operators. This includes that also the evolution kernels follow from the anomalous dimensions of these operators. Relations between different evolution kernels (especially the Altarelli-Parisi and the Brodsky-Lepage kernels) are derived and explicitly checked for the existing two-loop calculations of QCD. Technical basis of these results are support and analytically properties of the anomalous dimensions of light-ray operators obtained with the help of the α-representation of Green's functions.

References

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