two-component model by a $1p$ admixture. Assuming that the $1s$ quasihole momentum distribution is similar to the Dirac-Hartree wave function, it would appear that the continuum contribution to $E_m > 30$ MeV has a broader momentum distribution than the $1p_{3/2}$ wave function used in these two-component fits. Although part of this may be contributed by $1p$ fragmentation, much of the fitted $1p$ strength is probably a surrogate for multinucleon continuum. Recent SCGF estimates suggest that approximately $68\%$ of the correlated continuum is in partial waves with $\ell \leq 1$ [@Muther04]. No doubt higher partial waves begin to contribute to the continuum as $p_m$ increases and it is likely that the $\ell=1$ continuum is also broader than the $1p_{3/2}$ quasihole momentum distribution.

![ Contributions of $1p_{3/2}$ and $1s_{1/2}$ fitted to JLab data for $^{12}$C$(e,e^\prime p)$. In each panel the top set of curves shows the inclusive $10 \leq E_m \leq 80$ MeV bin scaled by a factor of 20, the middle set shows the $p$-shell bin with $15 \leq E_m \leq 25$ MeV, and the bottom set shows the $s$-shell bin with $30 \leq E_m \leq 50$ MeV scaled by a factor of 0.1. The solid curves show the total fit, 