We have studied the electron-momentum density distribution in Al using the
coincidence as well as the conventional high-resolution Compton scattering
technique. In order to interpret the results, corresponding band theory bas
ed computations of the electron momentum density (EMD) and the Compton prof
iles (CPs) have been carried out. Our focus here is on determining the size
of the break Z(F) in the EMD at the Fermi momentum. For this purpose, diff
erences between measurements and theoretical predictions are analyzed in te
rms of a simple model for describing electron correlation effects which are
missing from the independent particle band theory framework; the model inv
olves Z(F) as the only adjustable parameter. A good fit with the coincidenc
e measurements is obtained for Z(F) of about 0.7, while the CP data yields
Z(F) = 0.7 to 0.8. This study suggests that, in sharp contrast to the case
of Li where recent high-resolution Compton work indicates Z(F) approximate
to 0, the standard picture of the interacting electron gas is substantially
correct in Al. (C) 2000 Elsevier Science Ltd. All rights reserved.