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The evolution of the pion distribution amplitude in next-to-leading order is studied for a fixed and a running coupling constant. In both cases, the evolution provides a logarithmic modification in the end point region. Assuming a simple parametrization of the distribution amplitude at a scale of Q₀{~}0.5 GeV, it is shown numerically that these effects are large enough at Q{~}2 GeV that they have to be taken into account in the next-to-leading-order analysis for exclusive processes. Alternatively, by introducing a new distribution amplitude that evolves more smoothly, this logarithmic modification can be included in the hard-scattering part of the considered process.
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D. Müller (1995) studied this question.
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