We estimate the rate at which randomly stacked hard-sphere crystals transfo
rm into the thermodynamically stable face-centered cubic phase. As an input
for this estimate we need both the free-energy difference between bulk fac
e-centered cubic (fcc) and hexagonal close packed (hcp) phases, and the hcp
-fcc interfacial free energy. The latter quantity was computed using a latt
ice-switch Monte Carlo (MC) simulation method. We find the interfacial free
energy to be nonzero but extremely small: 26 +/- 6.1(05)kT/sigma(2),where
sigma is the particle diameter. The free energy difference between the bulk
phases was calculated using two different techniques. On the basis of our
simulation results we estimate that in hard-sphere colloidal suspensions mi
llimeter-sized randomly stacked crystal will anneal to form essentially pur
e fcc crystal on a time scale of months to years. (C) 1999 American Institu
te of Physics. [S0021-9606(99)51709-1].