\begin{table}%tB.1
%%\centering
\par
\caption{Fitting parameters for various cross sections.}\label{tab:fits}
%\centerline
{\small\begin{tabular}{lccccccccc}
\hline\hline
\multicolumn{1}{c}{Reaction} & \multicolumn{1}{c}{$A_0$} & \multicolumn{1}{c}{$A_1$} & \multicolumn{1}{c}{$A_2$} & \multicolumn{1}{c}{$A_3$} & \multicolumn{1}{c}{$A_4$} & \multicolumn{1}{c}{$A_5$} & \multicolumn{1}{c}{$A_6$} & \multicolumn{1}{c}{$A_7$} & \multicolumn{1}{c}{$A_8$}\\
\hline
$\sigma_{\rm{T,p},2s}$ & $-9.76244_1$ & $-8.02645$ & $-9.03528$ & $-6.82148_{-1}$ & 1.41138 & $-8.43613_{-3}$ & $-1.31162_{-1}$ & $-3.07135_{-1}$ & $3.60166_{-1}$\\
$\sigma_{\rm{T,p},2p}$ & $-9.47856_1$ & $-1.36982_1$ & $-7.48411$ & $-6.55633_{-1}$ & 1.08973 & $3.45255_{-1}$ & $-2.02178_{-1}$ & $-2.99212_{-1}$ & $2.88704_{-1}$ \\
$\sigma_{\rm{T,p},3s}$ & $-1.03831_{2}$ & $-5.12682$ & $-1.03311_{1}$ & $-2.36941_{-1}$ & $7.99974_{-1}$ & $6.55927_{-1}$ & $-2.64604_{-1}$ & $-6.82557_{-1}$ & $7.65819_{-1}$ \\
$\sigma_{\rm{T,p},3p}$ & $-1.04117_{2}$ & $-9.31370$ & $-1.09011_{1}$ & $2.72437_{-1}$ & $8.33272_{-1}$ & $9.72800_{-1}$ & $-3.40175_{-1}$ & $-8.21497_{-2}$ & $1.06280_{-1}$ \\
$\sigma_{\rm{T,p},3d}$ & $-1.06187_{2}$ & $-8.82542$ & $-1.05048_{1}$ & $9.29637_{-1}$ & $9.65598_{-1}$ & $7.99638_{-3}$ & $1.21539_{-1}$ & $-6.52001_{-1}$ & $4.15571_{-1}$ \\
$\sigma_{\rm{T,p},4s}$ & $-1.05018_{2}$ & $-5.69159$ & $-9.63683$ & $-8.65652_{-1}$ & 1.06090 & $9.33260_{-1}$ & $-8.64227_{-1}$ & $-1.30903_{-1}$ & $4.32513_{-1}$ \\
$\sigma_{\rm{T,p},4p}$ & $-1.06245_{2}$ & $-7.18909$ & $-1.07639_{1}$ & $1.84045_{-1}$ & 1.10514 & $3.64508_{-1}$ & $-2.30906_{-1}$ & $-4.14293_{-1}$ & $4.42254_{-1}$ \\
$\sigma_{\rm{T,p},4d}$ & $-1.08456_{2}$ & $-7.54281$ & $-1.11995_{1}$ & 1.15545 & $9.55810_{-1}$ & $9.05249_{-2}$ & $-1.37453_{-1}$ & $-4.09046_{-1}$ & $3.40271_{-1}$ \\
$\sigma_{\rm{T,p},4f}$ & $-1.10117_{2}$ & $-8.87472$ & $-1.00318_{1}$ & $3.41036_{-1}$ & 1.43444 & $1.22887_{-2}$ & $-4.35737_{-1}$ & $-7.29281_{-2}$ & $1.87428_{-1}$ \\
$\sigma_{\rm{E,e},2p}$ & $-7.67030_{1}$ & $-9.47539_{-1}$ & $-6.80475_{-1}$ & $2.77805_{-1}$ & $-1.18599_{-1}$ & $6.65029_{-2}$ & $-4.38768_{-2}$ & $2.20102_{-2}$ & $-2.24010_{-2}$ \\
$\sigma_{\rm{E,e},3p}$ & $-8.02681_{1}$ & $-1.00579$ & $-6.24421_{-1}$ & $2.59918_{-1}$ & $-1.13262_{-1}$ & $6.48909_{-2}$ & $-4.34274_{-2}$ & $2.15313_{-2}$ & $-2.31916_{-2}$ \\
$\sigma_{\rm{E,p},3s}$ & $-8.43473_{1}$ & 2.69180 & $-8.94871_{-1}$ & $-1.25347_{-1}$ & $-1.27427_{-1}$ & $2.16335_{-1}$ & $7.34001_{-3}$ & $-2.19545_{-1}$ & $-1.76763_{-1}$ \\
$\sigma_{\rm{E,p},3p}$ & $-8.10541_{1}$ & 2.27478 & $-4.95559_{-1}$ & $1.56523_{-2}$ & $2.45763_{-2}$ & $-1.29970_{-1}$ & $-2.66319_{-2}$ & $-6.13906_{-2}$ & $2.46815_{-1}$ \\
$\sigma_{\rm{E,p},3d}$ & $-8.22914_{1}$ & $7.43945_{-1}$ & $-5.04030_{-1}$ & $5.76290_{-2}$ & $8.40403_{-2}$ & $-3.04995_{-1}$ & $7.62616_{-2}$ & $2.56426_{-1}$ & $-3.65589_{-1}$ \\
\hline
\end{tabular}}
\smallskip
Note: $A_b$ is shorthand for $A \times 10^b$.  The following subscripts are used: ``T'' (charge transfer), ``E'' (impact excitation), ``p'' (proton) and ``e'' (electron).
\end{table}