\begin{table}%t1
  \caption{\label{tab:recipe-quantities}Quantities provided by the adjusted collision recipe.}
%\centerline
 {  \begin{tabular}{lp{88mm}ll}
    \hline\hline 
    Symbol & Description & \multicolumn{2}{c}{Energy scaling parameters in \eq{energy-parameter}}\\ 
    \cline{3-4} \\[-3.5mm]
           &             & Global       & Local  \\
    (1)    & (2)         & (3)          & (4)    \\
    \hline
    $f_{\rm miss}$ & Fraction of collisions that resulted in a miss$^a$        & ---                           & --  \\ 
    $N_{\rm f}$    & Mean number of large fragments                            & $N_{\rm tot}E_{\rm br}$ & $N_\mu E_{\rm br}$ \\
    $S_{\rm f}$    & Standard deviation of the $N_{\rm f}$                  & $N_{\rm tot}E_{\rm br}$ & $N_\mu E_{\rm br}$ \\
    $f_{\rm pwl}$  & The fraction of the mass in the small fragments component. Normalized to $N_{\rm tot}$ (global recipe) or $N_\mu$ (local recipe). & $N_{\rm tot}E_{\rm br}$ & $N_\mu E_{\rm br}$ \\
    $q$              & Exponent of the power-law distribution of small fragments  & $N_{\rm tot}E_{\rm br}$ & $N_\mu E_{\rm br}$ \\ 
    $C_\phi=\phi_\sigma/\phi_\sigma^{\rm ini}$ & Relative change of the geometrical filling factor.& $N_{\rm tot}E_{\rm roll}$ & $N_{\rm tot} E_{\rm roll}$ \\
    \hline
  \end{tabular}}
\par
  \smallskip
  {N{ote}: Columns (3)--(4) denote the energy scaling expressions used to obtain the dimensionless energy parameter, $\varepsilon$, see \eq{energy-parameter}. $^a$~Given as function of $a_{\rm out}/a_\sigma$ instead of $\phi_\sigma$, see \app{colltab}.}
  \end{table}