to the JLab data [@Dutta03] are shown in Fig. \[fig:Dutta\_nlsh\] using NLSH wave functions, EDAD1 optical potentials, and the CC2 current operator in Coulomb gauge. For the inclusive bin, these fits are slightly better than the corresponding EMA-noSV fits shown in Fig. \[fig:Dutta-EMAnoSV\] because full RDWIA calculations reproduce the left-right asymmetry better than the EMA-noSV approximation [@Kelly05a]. These fits for the $1p$ and $1s$ bins are significantly better than single-component fits because neither bin represents a pure single-particle configuration. The $1s$ contribution to the $1p$ bin fills in the minimum and rounds the peaks. Similarly the $1p$ contribution to the $1s$ bin broadens the momentum distribution — the reduced $1s$ component provides a better fit for small $p_m$ while the $1p$ component improves the fit to larger $p_m$. However, for $p_m > 200$ MeV/$c$ the data for both the $s$-shell and inclusive bins remain significantly above these two-component fits. Similar data for $^{16}$O$(e,e^\prime p)$ [@Liyanage01; @Fissum04] covering a broad range of missing energy show that for $p_m \gtrsim 150$ MeV/$c$ there is much more strength at large $E_m$ than can be attributed to single-nucleon knockout from the $s$-shell. The continuum fraction increases with $p_m$, which may be simulated in the 