The phase stability of the hcp, fcc, and bcc structures of Li is studi
ed using the pseudopotential density-functional total-energy calculati
on scheme. The order of the crystal energy at zero pressure is E(hcp)
< E(fcc) < E(bcc). The two closed-packed structures (fcc and hcp) are
fairly stable compared to the bcc structure for all volumes considered
, i.e., there is no pressure-induced bcc transition from either hcp or
fcc. The energy difference between hcp and fcc is very small and a hc
p-to-fcc transition occurs at a pressure of about 15 kbar. Unlike a pr
evious pseudopotential calculation, which predicted a fcc-to-bcc trans
ition, but no hcp-to-fcc transition, the present result on the transit
ions is in good agreement with existing all-electron calculations.