several low $Q^2$ experiments performed using quasiperpendicular kinematics. Except when noted otherwise, a normalization factor for each curve was obtained using a least-squares fit to the data for $|p_m| \leq 200$ MeV/$c$. Fig. \[EMA:Saclay\_kin2\] shows that the relativistic wave functions describe the data for the Saclay experiment with $T_p = 87$ MeV in quasiperpendicular kinematics better than the NIKHEF wave functions, which fall too rapidly with increasing $p_m$. The results shown in Fig. \[EMA:Tokyo\] for the Tokyo experiment with $Q^2 = 0.29$ (GeV/$c$)$^2$ are somewhat ambiguous: although the NLSH and HS wave functions give better fits to for $p_m \gtrsim 60$ MeV/$c$, particularly for the ground-state, none of the calculations can describe the enhancement at lower $p_m$ seen for the ground state or the dip for the $s$-state. The low $p_m$ bulge for the ground-state data seems somewhat implausible and it is likely that there were difficulties in cleanly separating the $1p$ and $1s$ contributions to the low $p_m$ data. Therefore, the $1p$ normalization for this set was fit to $50 \leq p_m \leq 200$ MeV/$c$. Similar calculations are also compared with the SLAC data for $Q^2 = 1.1$ (GeV/$c$)$^2$ in Fig. \[EMA:SLAC\]. We again find that the $p_m$ distribution 