\begin{table}%t2b
\par
\caption{\label{Table2b} Calculated \Fedisept\ fine structure levels, table not extended
to symmetries other than $J\pi=0^\re$. This symmetry has {\tt Nlv = 20} levels 
below~$\nu=11$ for the core ground state series: 3~Rydberg series ($\nu$~measured from the respective series limits, $E$~from the core ground state~$^2$P$_{3/2}$, the first limit).}
%\centering
\par
\begin{tabular}{rl@{\hspace{.5em}}r@{\hspace{.4em}}rrc@{\hspace{.6em}}rr@{}}
\hline\hline
\noalign{\smallskip}
{\tt I} &\multicolumn{3}{c}{{Level}} &$J$
 &$E$/Ry &\multicolumn{2}{r}{$\nu\quad \ SL\pi$}\\[.5ex]
\hline\noalign{\smallskip}
\multicolumn{8}{c}{\tt Nlv = 20,\qquad J pi =  0 e}\\[.5ex]
\hline 
\noalign{\smallskip}
 1 & 2s22p6  &         &       &   0      &$-$9.28398E+1 &       &$^1$S$^\re$\\
 2 & 2s22p5 &($^2$P$^\ro_{3/2}$) & 3p &0 &$-$3.62221E+1 & 2.825 &$^3$P$^\re$\\
 3 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 3p &0 &$-$3.48040E+1 & 2.844 &$^1$S$^\re$\\
 4 & 2s2p6  &($^2$S$    _{1/2}$) & 3s &0 &$-$2.90350E+1 & 2.731 &$^1$S$^\re$\\
 5 & 2s22p5 &($^2$P$^\ro_{3/2}$) & 4p &0 &$-$1.95296E+1 & 3.847 &$^3$P$^\re$\\
 6 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 4p &0 &$-$1.87056E+1 & 3.836 &$^1$S$^\re$\\
 7 & 2s22p5 &($^2$P$^\ro_{3/2}$) & 5p &0 &$-$1.22822E+1 & 4.850 &$^3$P$^\re$\\
 8 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 5p &0 &$-$1.14454E+1 & 4.830 &$^1$S$^\re$\\
 9 & 2s2p6  &($^2$S$    _{1/2}$) & 4s &0 &$-$1.10221E+1 & 3.734 &$^1$S$^\re$\\
10 & 2s22p5 &($^2$P$^\ro_{3/2}$) & 6p &0 &$-$8.44845E+0 & 5.849 &$^3$P$^\re$\\
11 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 6p &0 &$-$7.57469E+0 & 5.828 &$^1$S$^\re$\\
12 & 2s22p5 &($^2$P$^\ro_{3/2}$) & 7p &0 &$-$6.15891E+0 & 6.850 &$^3$P$^\re$\\
13 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 7p &0 &$-$5.26390E+0 & 6.828 &$^1$S$^\re$\\
14 & 2s22p5 &($^2$P$^\ro_{3/1}$) & 8p &0 &$-$4.68712E+0 & 7.852 &$^3$P$^\re$\\
15 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 8p &0 &$-$3.78258E+0 & 7.827 &$^1$S$^\re$\\
16 & 2s22p5 &($^2$P$^\ro_{3/2}$) & 9p &0 &$-$3.68406E+0 & 8.857 &$^3$P$^\re$\\
17 & 2s2p6  &($^2$S$    _{1/2}$) & 5s &0 &$-$3.19987E+0 & 4.733 &$^1$S$^\re$\\
18 & 2s22p5 &($^2$P$^\ro_{3/2}$) &10p &0 &$-$2.97673E+0 & 9.853 &$^3$P$^\re$\\
19 & 2s22p5 &($^2$P$^\ro_{1/2}$) & 9p &0 &$-$2.76993E+0 & 8.829 &$^1$S$^\re$\\
20 & 2s22p5 &($^2$P$^\ro_{3/2}$) &11p &0 &$-$2.45262E+0 &10.855 &$^3$P$^\re$\\
 \hline
\end{tabular}
\end{table}