  Inclusive electron scattering from nuclei at low momentum transfer
(corresponding to x>1) and moderate Q^2 is dominated by quasifree scattering
from nucleons. In the impulse approximation, the cross section can be directly
connected to the nucleon momentum distribution via the scaling function F(y).
The breakdown of the y-scaling assumptions in certain kinematic regions have
prevented extraction of nucleon momentum distributions from such a scaling
analysis. With a slight modification to the y-scaling assumptions, it is found
that scaling functions can be extracted which are consistent with the
expectations for the nucleon momentum distributions.
