\begin{table}%t2 \caption{\label{tab_rad}Radiative decay rates ($A_{i,j}$ for $i\leftarrow j$ transition in units of~s$^{-1}$) for transitions to the ground level.} \small%\centerline { \begin{tabular}{ccccc} \hline\hline &&&& \\[-8pt] {\rm low} & {\rm upper} & AS${^a}$ & ZS94${^b}$ & NIST${^c}$ \\ \hline &&&& \\[-8pt] 1 & 3 & 3.267(05)$^d$ & 3.020(05) & 2.99(05) \\ 1 & 6 & 1.964(09) & 1.850(09) & 1.91(09) \\ 1 & 8 & 5.185(09) & 4.940(09) & 5.07(09) \\ 1 & 9 & 9.271(09) & 8.850(09) & 9.23(09) \\ 1 & 10 & 2.781(09) & 2.740(09) & 2.78(09) \\ 1 & 16 & 5.509(10) & 4.386(10) & \\ 1 & 19 & 8.032(11) & 7.378(11) & 8.15(11) \\ 1 & 26 & 1.262(11) & 1.063(11) & \\ 1 & 27 & 3.009(10) & 2.922(10) & \\ 1 & 28 & 1.586(11) & 1.163(11) & 2.66(11) \\ 1 & 29 & 5.266(10) & 3.723(10) & 7.27(10) \\ 1 & 32 & 1.582(09) & 1.293(09) & \\ 1 & 33 & 5.395(08) & 6.594(08) & \\ 1 & 34 & 3.205(08) & 2.747(08) & \\ 1 & 36 & 3.433(11) & 3.217(11) & 3.61(11) \\ 1 & 41 & 1.290(11) & 1.400(11) & 1.29(11) \\ 1 & 58 & 6.518(10) & 9.096(10) & \\ 1 & 59 & 2.365(09) & 1.386(09) & \\ 1 & 60 & 4.053(10) & 4.827(10) & \\ 1 & 62 & 2.720(10) & 1.353(10) & 2.15(10) \\ 1 & 63 & 3.811(08) & 2.987(08) & \\ 1 & 64 & 4.958(06) & 6.865(06) & \\ 1 & 70 & 2.789(10) & 3.705(10) & \\ 1 & 71 & 8.517(09) & 1.103(10) & \\ 1 & 79 & 4.453(09) & 6.434(09) & \\ 1 & 95 & 9.367(08) & 1.969(09) & \\ 1 & 96 & 6.778(08) & 1.574(09) & \\ 1 & 98 & 6.217(08) & 7.689(08) & \\ 1 & 100 & 4.124(09) & 7.050(09) & \\ 1 & 108 & 2.976(09) & 3.747(09) & \\ 1 & 111 & 1.482(10) & 3.010(10) & \\ 1 & 115 & 8.574(09) & 1.538(10) & \\ 1 & 119 & 9.798(09) & 1.579(10) & \\ 1 & 120 & 2.011(09) & 3.116(09) & \\ 1 & 121 & 1.649(09) & 5.421(09) & \\ 1 & 125 & 1.955(09) & 4.028(09) & \\ \hline \end{tabular}} \medskip $^{a}$ {\sc autostructure} (present work); $^{b}$ Zhang \& Sampson (\cite{ZS94}); $^{c}$~NIST~v3 (from Cavalcanti et~al. \cite{CLT00}); $^{d}$ ($m$) denotes $\times10^m$. \end{table}