We employ the local-density approximation to derive the spectral funct
ion P(k, E) of finite nuclei. For various densities of nuclear matter
we calculate P(k, E), and split it into the single-particle and correl
ated parts. For finite nuclei P(k, E) is calculated by combining the n
uclear-matter correlated part, evaluated in local-density approximatio
n, with the finite-nucleus single-particle part obtained from mean-fie
ld calculations or (e, e'p) experiments. These spectral functions are
used to calculate cross sections for inclusive electron-nucleus scatte
ring at large momentum transfer. The recoil-nucleon final-state intera
ction is treated in the local-density approximation as well.