\begin{table}%t6
\caption{\label{Table6} Comparison of BPRM calculations for decay $A^{\rm E1}(j,1)$
to the \Fedisept\ ground state $C_1T_1 =$~2s$^2$2p$^6~^1$S$_0$
with other work.}
%\centering
\par
\begin{tabular}{r@{\hspace{.9em}}l@{\hspace{.4em}}ll@{\hspace{.7em}}l@{}}
\hline\hline
\noalign{\smallskip}
\ $j$: &\ \ $C_j$ &$T_j$ 
 &&\multicolumn{1}{l}{\normalsize\ $A(s^{-1})$}\\[-.5em]
& & &\multicolumn{1}{c}{BPRM} & \multicolumn{1}{c}{Others}\\
 \noalign{\smallskip}
\hline
 \noalign{\smallskip}
 3: &2s$^2$2p$^5$3s &$^1$P$_1^\ro$  &7.96(11)
 & $8.28(11)^{a}, 8.01(11)^{b}, 7.75(11)^{c}$\\
& & & &$8.38(11)^{d}, 8.30(11)^{e}, 9.40(11)^\ddagger$\\
 5: &2s$^2$2p$^5$3s & $^3$P$_1^\ro$ & 9.35(11)
 & $9.76(11)^{a}, 9.44(11)^{b}, 9.09(11)^{c}$\\
& & & &$9.63(11)^{d}, 9.34(11)^{\rm e}, 8.00(11)^\ddagger$\\[.3ex]
17: &2s$^2$2p$^5$3d & $^3$P$_1^\ro$ & 7.58(10)
 & $9.19(10)^{a}, 8.27(10)^{b}, 7.77(10)^{c}$\\
& & & &$9.42(10)^{d}, 9.00(10)^{e}, 8.89(10)^\ddagger$\\[.3ex]
23: &2s$^2$2p$^5$3d & $^3$D$_1^\ro$ & 5.93(12)
 & $6.33(12)^{a}, 5.68(12)^{b}, 5.23(12)^{c}$\\
& & & &$6.01(12)^{d}, 6.01(12)^{e}, 5.72(12)^\ddagger$\\
27: &2s$^2$2p$^5$3d & $^1$P$_1^\ro$ & 2.28(13)
 & $2.24(13)^{a}, 2.64(13)^{b}, 2.44(13)^{c}$\\
& & & &$2.47(13)^{d}, 2.28(13)^{e}, 2.52(13)^\ddagger$\\
31: &2s2p$^6$3p & $^3$P$_1^\ro$ & 4.03(11)
 & $4.51(11)^{a}, 3.66(11)^{b}$\\
& & & &$4.12(11)^{d}, 3.40(11)^{e}, 3.52(11)^\ddagger$\\
33: &2s2p$^6$3p & $^1$P$_1^\ro$ & 3.30(12)
 & $3.34(12)^{a}, 3.21(12)^{b}$\\
& & & &$3.29(12)^{d}, 3.30(12)^{e}, 3.25(12)^\ddagger$\\[.5ex]
\hline
\noalign{\smallskip}
\multicolumn{5}{l}{{$^{a}$}~Safronova \etal (\cite{Safronova2001}), {$^{b}$}~Bhatia \& Doschek (\cite{Bhatia1992}),}\\
\multicolumn{5}{l}{{$^{c}$}~Cornille \etal (\cite{Cornille1994}), {$^{d}$}~ present MCDF, {$^{e}$}~ NIST,}\\
\multicolumn{5}{l}{$^\ddagger$  \sss\ with {\it all\/} magnetic
FS-components.}\\
\hline
\end{tabular}
\end{table}