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gg splitting function. This error results in a somewhat more rapid evolution of the gluon and sea-quark densities at small x. In addition, a next-to-leading order contribution in the quark-to-charm splitting function was missing, affecting essentially only the evolution of the charm quark density. For the process of interest to us at RHIC energies, dominated as it is by intermediate and large x and having little sensitivity to charm, the final quantitative differences are insignificant.
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