Final-state interactions (FSI) are important for both inclusive and exclusive lepton-nucleus interactions.
We show how such an approach may lead to different results for outgoing nucleons compared to a full calculation. We then avoid this problem of factorization, and perform a consistent comparison of proton FSI in the NEUT cascade model and in distorted-wave calculations that successfully describe exclusive (e,e^\prime p) reactions. We show that the cascade and distorted wave calculations agree for high nucleon energies but differ greatly for small energies.
CTGWG