We examine the possibility of quasicrystalline metastable states for o
ne-and two-component hard-sphere solids, systems whose excess free ene
rgies are entirely entropic. The investigations are carried out using
the self-consistent modified weighted density approximation of density
functional theory as applied to inhomogeneous systems. By a method en
tirely formulated in reciprocal space, we find that the best quasicrys
talline phases have significantly higher free energies than the crysta
lline or liquid states. These results indicate that quasicrystals prob
ably cannot be stabilized entirely by dynamic entropy.