Charm asymmetries in fixed-target hadroproduction experiments are sensitive
to power corrections to the QCD factorization theorem for heavy quark
production. A power correction called heavy-quark recombination has recently
been proposed to explain these asymmetries. In heavy-quark recombination, a
light quark or antiquark participates in a hard scattering which produces a
charm-anticharm quark pair. The light quark or antiquark emerges from the
scattering with small momentum in the rest frame of the charm quark, and
together they hadronize into a charm particle. The cross section for this
process can be calculated within perturbative QCD up to an overall
normalization. Heavy-quark recombination explains the observed D meson and
\Lambda_c asymmetries with a minimal set of universal nonperturbative
parameters.Comment: 10 pages, LaTeX, 8 figures, talk given at Strange Quark Matter 2003
Conference, Atlantic Beach, North Carolina, Mar 12-17, to be published in J.
Phys.