Recently there has been renewed interest in implementations of density
-functional theory for solids using various types of localized basis s
ets, including atom-centered Gaussian-type functions. While such metho
ds are clearly well adapted to most insulating and semiconducting syst
ems, one might expect them to give a less-than-optimal description of
metals relative to plane-wave-type methods. Nevertheless, several succ
essful applications of local-basis methods to metals have recently bee
n reported. Here, we report an application of our Gaussian linear comb
ination of atomic orbitals (LCAO) code to some extremely free-electron
-like metals, namely, the alkali metals Li, Na, and K. In agreement wi
th other calculations (both local and plane wave) we find that the loc
al-density approximation (LDA) lattice constants are relatively poor (
similar to-3% from experiment for the alkali metals versus +/-1% for m
any other solids) and that the LDA bulk moduli are similar to 30% too
high. We find that the Perdew-Burke-Enzerhof (PBE) version of the gene
ralized-gradient approximation (GGA) corrects most of this error, in a
greement with earlier calculations using similar GGA functionals. The
Becke-Lee-Yang-Parr GGA functional gives similar results for the alkal
i-metal equations of state but is found to overcorrect the errors of t
he LDA for the cohesive energies, for which the PBE functional is in b
etter agreement with experiment. Our results indicate that the Gaussia
n-LCAO method should be able to give accurate results for nearly any c
rystalline solid, since it succeeds even where it would be expected to
have the most difficulty. [S0163-1829(98)07919-3].