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MM_Si-2013-11-10.tex
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\begin{table*}
\begin{center}
\caption{
Laboratory data for transitions of Si of interest for quasar absorption-line varying-$\alpha$ studies described in \Sref{ssec:Si}. See \Sref{ssec:tabs} for full descriptions of each column.
}
\label{tab:Si}\vspace{-0.5em}
{\footnotesize
\begin{tabular}{:l;l;c;l;c;l;c;l;l;c;c;c;c}\hline
\multicolumn{1}{c}{Ion}&
\multicolumn{1}{c}{Tran.}&
\multicolumn{1}{c}{$A$}&
\multicolumn{1}{c}{$\omega_0$}&
\multicolumn{1}{c}{$X$}&
\multicolumn{1}{c}{$\lambda_0$}&
\multicolumn{1}{c}{$\delta v$}&
\multicolumn{1}{c}{Lower state}&
\multicolumn{1}{c}{Upper state}&
\multicolumn{1}{c}{ID}&
\multicolumn{1}{c}{IP$^-$, IP$^+$}&
\multicolumn{1}{c}{$f$ or {\it \%}}&
\multicolumn{1}{c}{$q$}\\
&
&
&
\multicolumn{1}{c}{[cm$^{-1}$]}&
&
\multicolumn{1}{c}{[\AA]}&
\multicolumn{1}{c}{[m\,s$^{-1}$]}&
&
&
&
\multicolumn{1}{c}{[eV]}&
&
\multicolumn{1}{c}{[cm$^{-1}$]}\\
\hline
Si{\sc \,ii} & 1526 & 28.0855 & 65500.4538(7)$^{a}$ & 0 & 1526.706980(16) & 3.2 & $3\rm{s}^23\rm{p}~^2\rm{P}_{1/2}^{\rm o} $ & $3\rm{s}^24\rm{s}~^2\rm{S}_{1/2} $ & Si$^2_{2}$ & 8.15, 16.35 & 0.133 & $ 47^{b}(4) $\\
\rowstyle{\itshape} & & 30 & 65500.42585$^{b}$ & 3 & 1526.7076312 & & $ $ & $ $ & & & 3.087\% & $ ^{} $\\
\rowstyle{\itshape} & & 29 & 65500.43980$^{b}$ & 3 & 1526.7073061 & & $ $ & $ $ & & & 4.683\% & $ ^{} $\\
\rowstyle{\itshape} & & 28 & 65500.45545$^{b}$ & 3 & 1526.7069415 & & $ $ & $ $ & & & 92.230\% & $ ^{} $\\
& 1808 & 28.0855 & 55309.3404(4)$^{a}$ & 0 & 1808.012883(13) & 2.2 & $ $ & $3\rm{s}3\rm{p}^2~^2\rm{D}_{3/2} $ & Si$^2_{4}$ & & 0.00208 & $ 526^{b}(16) $\\
\rowstyle{\itshape} & & 30 & 55309.49010$^{b}$ & 3 & 1808.0079895 & & $ $ & $ $ & & & 3.087\% & $ ^{} $\\
\rowstyle{\itshape} & & 29 & 55309.41403$^{b}$ & 3 & 1808.0104763 & & $ $ & $ $ & & & 4.683\% & $ ^{} $\\
\rowstyle{\itshape} & & 28 & 55309.33165$^{b}$ & 3 & 1808.0131691 & & $ $ & $ $ & & & 92.230\% & $ ^{} $\\
Si{\sc \,iv} & 1393 & 28.0855 & 71748.355(2)$^{a}$ & 0 & 1393.760177(39) & 8.4 & $2\rm{p}^63\rm{s}~^2\rm{S}_{1/2} $ & $2\rm{p}^63\rm{p}~^2\rm{P}_{3/2}^{\rm o} $ & Si$^4_{1}$ & 33.49, 45.14 & 0.513 & $ 823^{c}(2) $\\
\rowstyle{\itshape} & & 30 & 71748.5517$^{d}$ & 3 & 1393.7563570 & & $ $ & $ $ & & & 3.087\% & $ ^{} $\\
\rowstyle{\itshape} & & 29 & 71748.4513$^{d}$ & 3 & 1393.7583075 & & $ $ & $ $ & & & 4.683\% & $ ^{} $\\
\rowstyle{\itshape} & & 28 & 71748.3435$^{d}$ & 3 & 1393.7604003 & & $ $ & $ $ & & & 92.230\% & $ ^{} $\\
& 1402 & 28.0855 & 71287.376(2)$^{a}$ & 0 & 1402.772912(39) & 8.4 & $ $ & $2\rm{p}^63\rm{p}~^2\rm{P}_{1/2}^{\rm o} $ & Si$^4_{2}$ & & 0.254 & $ 361^{c}(2) $\\
\rowstyle{\itshape} & & 30 & 71287.5743$^{d}$ & 3 & 1402.7690089 & & $ $ & $ $ & & & 3.087\% & $ ^{} $\\
\rowstyle{\itshape} & & 29 & 71287.4731$^{d}$ & 3 & 1402.7710015 & & $ $ & $ $ & & & 4.683\% & $ ^{} $\\
\rowstyle{\itshape} & & 28 & 71287.3644$^{d}$ & 3 & 1402.7731393 & & $ $ & $ $ & & & 92.230\% & $ ^{} $\\
\hline
\end{tabular}
}
{\footnotesize References:
$^{a}$\citet{Griesmann:2000:L113};
$^{b}$This work;
$^{c}$\citet{Dzuba:2007:062510};
$^{d}$\citet{Berengut:2003:022502}.}
\end{center}
\end{table*}