39$ MeV for $^{12}$C. Lapikás [[*et al.* ]{}]{}obtained slightly different parameters for $b$ and $E_{1s}$ by fitting the Tokyo data, but the effect upon $S_{1s}$ is insignificant. Thus, one would expect approximately $11\%$ of the $1s$ strength to be broadly distributed above 80 MeV missing energy, which is consistent with the depletion factor attributed to short-range correlations. Therefore, in the absence of background, the $1s$ spectroscopic factor deduced from a fitted normalization factor would be $$\label{eq:1s}
S_{1s} = 2 N_{1s}(E_\text{min},E_\text{max})
\frac{ \int_0^\infty L_{1s}(E_m) dE_m } 
{ \int_{E_\text{min}}^{E_\text{max}} L_{1s}(E_m) dE_m }$$

  --------------------------- --------- ------------------ ------------------ ------- --------------- --------------------------------------------------------
  data set                        $E_0$   $\Delta E_m(1p)$   $\Delta E_m(1s)$   $T_p$           $Q^2$ notes
                                    MeV                MeV                MeV     MeV   (GeV/$c$)$^2$ 
  Tokyo [@Nakamura76]               700               6-30              21-66     159            0.29 
                                    700                                 21-66     136                 
  Saclay [@Mougey76]                497              15-22              30-50      87            0.16 
  Saclay [@Bernheim82]              500              15-22                 NA      99            0.18 constant $(\omega,\bm{q})$
  Saclay [@Bernheim82]              500              15-22                 NA      99       0.09-0.32 parallel; $1s$ not available
  NIKHEF [@vdSteenhoven88a]     285-481              15-22              30-39      70       0.02-0.26 parallel
  SLAC [@Makins94]                 2015              15-25              30-80     600            1.11 $1s$ not radiatively unfolded
  JLab [@Dutta03]                  2445              15-25              30-50     350            0.64 inclusive bin with $10 \leq E_m \leq 80$ MeV available
                                   2445                                           700            1.28 
                                   3245                                           970            1.84 
  --------------------------- --------- ------------------ ------------------ ------- --------------- --------------------------------------------------------

  : Summary 