Abstract
A previous calculation of the dielectric matrix in aluminum in the static limit is extended to include the frequency dependence. Exchange and correlation corrections to the random-phase results are studied according to three different approximations. The values of Im[ε1(k,ω)]11, responsible for the electron-energy-loss cross sections, are computed and compared with the experimental results of Petri and Otto. The results do not depend significantly on the form of exchange-correlation corrections employed.