
 \documentclass[referee]{aa} % for a referee version
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%\documentclass{aa}
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 \usepackage{dcolumn}
 \addtocounter{table}{3}

\begin{document}

\begin{table}[htbp]
 \caption{Calculated $\Delta F=+1$ hyperfine components (MHz) and relative intensities of
 submillimeter-wave transitions of N$_2$D$^+$}\label{list1}
 \centering
 \begin{tabular}{ccccccD{.}{.}{3}D{.}{.}{3}|ccccccD{.}{.}{3}D{.}{.}{3}}

 \hline \noalign{\smallskip}
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} &
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
  \multicolumn{6}{c}{$J=7 \leftarrow 6$} & 539\,682.081(32) & & \multicolumn{6}{c}{$J=8 \leftarrow 7$} & 616\,749.977(56) & \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
 7 &  6 &  5 &  6 &  5 &  4 & 539\,682.029 & 0.077 & 8 &  7 &  6 &  7 &  6 &  5 & 616\,749.934 & 0.081 \cr
 7 &  6 &  6 &  6 &  5 &  5 & 539\,682.038 & 0.091 & 8 &  7 &  7 &  7 &  6 &  6 & 616\,749.942 & 0.094 \cr
 7 &  6 &  7 &  6 &  5 &  6 & 539\,682.056 & 0.109 & 8 &  7 &  8 &  7 &  6 &  7 & 616\,749.957 & 0.109 \cr
 7 &  7 &  6 &  6 &  6 &  5 & 539\,682.074 & 0.092 & 8 &  8 &  7 &  7 &  7 &  6 & 616\,749.969 & 0.095 \cr
 7 &  7 &  7 &  6 &  6 &  6 & 539\,682.078 & 0.107 & 8 &  8 &  8 &  7 &  7 &  7 & 616\,749.974 & 0.108 \cr
 7 &  7 &  8 &  6 &  6 &  7 & 539\,682.096 & 0.123 & 8 &  8 &  9 &  7 &  7 &  8 & 616\,749.989 & 0.122 \cr
 7 &  8 &  7 &  6 &  7 &  6 & 539\,682.098 & 0.109 & 8 &  9 &  8 &  7 &  8 &  7 & 616\,749.991 & 0.110 \cr
 7 &  8 &  8 &  6 &  7 &  7 & 539\,682.106 & 0.124 & 8 &  9 &  9 &  7 &  8 &  8 & 616\,749.999 & 0.123 \cr
 7 &  8 &  9 &  6 &  7 &  8 & 539\,682.119 & 0.141 & 8 &  9 & 10 &  7 &  8 &  9 & 616\,750.010 & 0.137 \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
  \multicolumn{6}{c}{$J=9 \leftarrow 8$} & 693\,806.055(88) & & \multicolumn{6}{c}{$J=10 \leftarrow 9$} & 770\,848.837(131) & \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
 9 &  8 &  7 &  8 &  7 &  6 & 693\,806.018 & 0.085 & 10 &  9 &  8 &  9 &  8 &  7 & 770\,848.804 & 0.088 \cr
 9 &  8 &  8 &  8 &  7 &  7 & 693\,806.026 & 0.096 & 10 &  9 &  9 &  9 &  8 &  8 & 770\,848.812 & 0.098 \cr
 9 &  8 &  9 &  8 &  7 &  8 & 693\,806.038 & 0.110 & 10 &  9 & 10 &  9 &  8 &  9 & 770\,848.823 & 0.110 \cr
 9 &  9 &  8 &  8 &  8 &  7 & 693\,806.047 & 0.097 & 10 & 10 &  9 &  9 &  9 &  8 & 770\,848.828 & 0.098 \cr
 9 &  9 &  9 &  8 &  8 &  8 & 693\,806.052 & 0.108 & 10 & 10 & 10 &  9 &  9 &  9 & 770\,848.835 & 0.109 \cr
 9 &  9 & 10 &  8 &  8 &  9 & 693\,806.065 & 0.121 & 10 & 10 & 11 &  9 &  9 & 10 & 770\,848.846 & 0.120 \cr
 9 & 10 &  9 &  8 &  9 &  8 & 693\,806.066 & 0.110 & 10 & 11 & 10 &  9 & 10 &  9 & 770\,848.846 & 0.110 \cr
 9 & 10 & 10 &  8 &  9 &  9 & 693\,806.074 & 0.122 & 10 & 11 & 11 &  9 & 10 & 10 & 770\,848.854 & 0.121 \cr
 9 & 10 & 11 &  8 &  9 & 10 & 693\,806.084 & 0.134 & 10 & 11 & 12 &  9 & 10 & 11 & 770\,848.864 & 0.132 \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
  \multicolumn{6}{c}{$J=11 \leftarrow 10$} & 847\,876.846(183) & & \multicolumn{6}{c}{$J=12 \leftarrow 11$} & 924\,888.605(247) & \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
 11 & 10 &  9 & 10 &  9 &  8 & 847\,876.816 & 0.090 & 12 & 11 & 10 & 11 & 10 &  9 & 924\,888.578 & 0.092 \cr
 11 & 10 & 10 & 10 &  9 &  9 & 847\,876.824 & 0.099 & 12 & 11 & 11 & 11 & 10 & 10 & 924\,888.586 & 0.101 \cr
 11 & 10 & 11 & 10 &  9 & 10 & 847\,876.834 & 0.110 & 12 & 11 & 12 & 11 & 10 & 11 & 924\,888.595 & 0.110 \cr
 11 & 11 & 10 & 10 & 10 &  9 & 847\,876.838 & 0.100 & 12 & 12 & 11 & 11 & 11 & 10 & 924\,888.597 & 0.101 \cr
 11 & 11 & 11 & 10 & 10 & 10 & 847\,876.844 & 0.109 & 12 & 12 & 12 & 11 & 11 & 11 & 924\,888.604 & 0.110 \cr
 11 & 12 & 11 & 10 & 11 & 10 & 847\,876.854 & 0.110 & 12 & 13 & 12 & 11 & 12 & 11 & 924\,888.613 & 0.110 \cr
 11 & 11 & 12 & 10 & 10 & 11 & 847\,876.855 & 0.120 & 12 & 12 & 13 & 11 & 11 & 12 & 924\,888.614 & 0.119 \cr
 11 & 12 & 12 & 10 & 11 & 11 & 847\,876.862 & 0.120 & 12 & 13 & 13 & 11 & 12 & 12 & 924\,888.620 & 0.119 \cr
 11 & 12 & 13 & 10 & 11 & 12 & 847\,876.871 & 0.130 & 12 & 13 & 14 & 11 & 12 & 13 & 924\,888.629 & 0.129 \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
\end{tabular}
\end{table}

\begin{table}[htbp]
 \caption{Calculated hyperfine components (MHz)$^{\mathrm{a}}$ and relative intensities of the $J=2 \leftarrow 1$
 and $J=3 \leftarrow 2$ transitions of N$_2$D$^+$}\label{list2}
 \centering
 \begin{tabular}{ccccccD{.}{.}{3}D{.}{.}{3}|ccccccD{.}{.}{3}D{.}{.}{3}}

 \hline \noalign{\smallskip}
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} &
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
2 & 2 & 2 & 1 & 2 & 1 & 154\,214.845 & 0.002     & 3 & 3 & 2 & 2 & 3 & 2 & 231\,319.945 & 0.010 \cr
2 & 2 & 2 & 1 & 2 & 3 & 154\,215.040 & 0.004     & 3 & 3 & 4 & 2 & 3 & 4 & 231\,319.995 & 0.017 \cr
2 & 2 & 1 & 1 & 2 & 1 & 154\,215.168 & 0.020     & 3 & 3 & 3 & 2 & 3 & 3 & 231\,320.017 & 0.007 \cr
2 & 2 & 3 & 1 & 2 & 3 & 154\,215.288 & 0.039     & 3 & 2 & 2 & 2 & 1 & 2 & 231\,321.253 & 0.015 \cr
2 & 2 & 2 & 1 & 2 & 2 & 154\,215.331 & 0.011     & 3 & 2 & 2 & 2 & 1 & 1 & 231\,321.456 & 0.048 \cr
2 & 1 & 1 & 1 & 0 & 1 & 154\,215.425 & 0.036     & 3 & 2 & 1 & 2 & 1 & 0 & 231\,321.499 & 0.022 \cr
2 & 2 & 3 & 1 & 2 & 2 & 154\,215.579 & 0.005     & 3 & 4 & 4 & 2 & 3 & 4 & 231\,321.530 & 0.007 \cr
2 & 1 & 2 & 1 & 0 & 1 & 154\,215.628 & 0.062     & 3 & 3 & 3 & 2 & 2 & 3 & 231\,321.547 & 0.014 \cr
2 & 2 & 1 & 1 & 2 & 2 & 154\,215.653 & 0.003     & 3 & 2 & 3 & 2 & 1 & 2 & 231\,321.617 & 0.094 \cr
2 & 1 & 0 & 1 & 0 & 1 & 154\,215.888 & 0.013     & 3 & 3 & 3 & 2 & 2 & 2 & 231\,321.795 & 0.089 \cr
2 & 2 & 2 & 1 & 1 & 1 & 154\,216.754 & 0.066     & 3 & 3 & 2 & 2 & 2 & 1 & 231\,321.908 & 0.061 \cr
2 & 3 & 3 & 1 & 2 & 3 & 154\,216.818 & 0.013     & 3 & 3 & 4 & 2 & 2 & 3 & 231\,321.914 & 0.125 \cr
2 & 2 & 2 & 1 & 1 & 2 & 154\,216.889 & 0.027     & 3 & 4 & 4 & 2 & 3 & 3 & 231\,321.918 & 0.136 \cr
2 & 2 & 1 & 1 & 1 & 1 & 154\,217.076 & 0.012     & 3 & 4 & 3 & 2 & 3 & 2 & 231\,321.919 & 0.101 \cr
2 & 3 & 3 & 1 & 2 & 2 & 154\,217.109 & 0.143     & 3 & 2 & 1 & 2 & 1 & 1 & 231\,321.961 & 0.019 \cr
2 & 3 & 2 & 1 & 2 & 1 & 154\,217.131 & 0.088     & 3 & 4 & 5 & 2 & 3 & 4 & 231\,321.966 & 0.175 \cr
2 & 2 & 3 & 1 & 1 & 2 & 154\,217.137 & 0.112     & 3 & 3 & 2 & 2 & 2 & 2 & 231\,322.231 & 0.007 \cr
2 & 3 & 4 & 1 & 2 & 3 & 154\,217.206 & 0.200     & 3 & 4 & 3 & 2 & 3 & 3 & 231\,322.426 & 0.010 \cr
2 & 2 & 1 & 1 & 1 & 0 & 154\,217.502 & 0.031     & 3 & 2 & 2 & 2 & 2 & 1 & 231\,324.012 & 0.002 \cr
2 & 3 & 2 & 1 & 2 & 2 & 154\,217.617 & 0.021     & 3 & 2 & 2 & 2 & 2 & 3 & 231\,324.086 & 0.002 \cr
2 & 1 & 2 & 1 & 2 & 3 & 154\,218.120 & 0.003     & 3 & 2 & 2 & 2 & 2 & 2 & 231\,324.334 & 0.011 \cr
2 & 1 & 1 & 1 & 1 & 1 & 154\,219.631 & 0.010     & 3 & 2 & 3 & 2 & 2 & 3 & 231\,324.450 & 0.014 \cr
2 & 1 & 1 & 1 & 1 & 2 & 154\,219.766 & 0.013     & 3 & 2 & 1 & 2 & 2 & 1 & 231\,324.517 & 0.004 \cr
2 & 1 & 2 & 1 & 1 & 1 & 154\,219.834 & 0.014     & 3 & 2 & 3 & 2 & 2 & 2 & 231\,324.698 & 0.002 \cr
2 & 1 & 2 & 1 & 1 & 2 & 154\,219.969 & 0.031     & 3 & 2 & 1 & 2 & 2 & 2 & 231\,324.839 & 0.002 \cr
2 & 1 & 1 & 1 & 1 & 0 & 154\,220.058 & 0.006     &   &   &   &   &   &   &              &       \cr
2 & 1 & 0 & 1 & 1 & 1 & 154\,220.094 & 0.008     &   &   &   &   &   &   &              &       \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
\end{tabular}
\begin{list}{}{}
\item[$^{\mathrm{a}}$] estimated uncertainties based on propagation of the  spectroscopic constants' errors
are 8 and 10 kHz for the $J=2 \leftarrow 1$ and $J=3 \leftarrow 2$ transitions, respectively
\end{list}
\end{table}

\begin{table}[htbp]
 \caption{Calculated hyperfine components (MHz)$^{\mathrm{a}}$ and relative intensities of the $J=4 \leftarrow 3$
 transition of N$_2$D$^+$}\label{list3}
 \centering
 \begin{tabular}{ccccccD{.}{.}{3}D{.}{.}{3}}

 \hline \noalign{\smallskip}
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
  \multicolumn{8}{c}{$\Delta F=+1$}\cr
 4 &  3 &  3 &  3 &  2 &  2 & 308\,422.092 & 0.069 \cr
 4 &  3 &  2 &  3 &  2 &  1 & 308\,422.094 & 0.048 \cr
 4 &  3 &  4 &  3 &  2 &  3 & 308\,422.157 & 0.103 \cr
 4 &  4 &  4 &  3 &  3 &  3 & 308\,422.233 & 0.098 \cr
 4 &  4 &  3 &  3 &  3 &  2 & 308\,422.263 & 0.075 \cr
 4 &  4 &  5 &  3 &  3 &  4 & 308\,422.290 & 0.126 \cr
 4 &  5 &  4 &  3 &  4 &  3 & 308\,422.296 & 0.105 \cr
 4 &  5 &  5 &  3 &  4 &  4 & 308\,422.301 & 0.131 \cr
 4 &  5 &  6 &  3 &  4 &  5 & 308\,422.331 & 0.160 \cr
  \multicolumn{8}{c}{$\Delta F=0$}\cr
 4 &  4 &  3 &  3 &  4 &  3 & 308\,420.289 & 0.006 \cr
 4 &  4 &  5 &  3 &  4 &  5 & 308\,420.320 & 0.009 \cr
 4 &  4 &  4 &  3 &  4 &  4 & 308\,420.332 & 0.005 \cr
 4 &  3 &  3 &  3 &  2 &  3 & 308\,421.728 & 0.008 \cr
 4 &  5 &  5 &  3 &  4 &  5 & 308\,421.865 & 0.005 \cr
 4 &  4 &  4 &  3 &  3 &  4 & 308\,421.866 & 0.008 \cr
 4 &  3 &  2 &  3 &  2 &  2 & 308\,422.599 & 0.010 \cr
 4 &  4 &  3 &  3 &  3 &  3 & 308\,422.699 & 0.005 \cr
 4 &  5 &  4 &  3 &  4 &  4 & 308\,422.804 & 0.006 \cr
 4 &  3 &  3 &  3 &  3 &  3 & 308\,424.631 & 0.007 \cr
 4 &  3 &  4 &  3 &  3 &  4 & 308\,424.693 & 0.008 \cr
 4 &  3 &  2 &  3 &  3 &  2 & 308\,424.703 & 0.003 \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
\end{tabular}
\begin{list}{}{}
\item[$^{\mathrm{a}}$] the estimated uncertainty based on propagation of the  spectroscopic constants' errors
is 10 kHz
\end{list}
\end{table}

\begin{table}[htbp]
 \caption{Calculated hyperfine components (MHz)$^{\mathrm{a}}$ and relative intensities of the $J=5 \leftarrow 4$
 transition of N$_2$D$^+$}\label{list4}
 \centering
 \begin{tabular}{ccccccD{.}{.}{3}D{.}{.}{3}}

 \hline \noalign{\smallskip}
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
  \multicolumn{8}{c}{$\Delta F=+1$}\cr
 5 &  4 &  3 &  4 &  3 &  2 & 385\,516.647 & 0.062 \cr
 5 &  4 &  4 &  4 &  3 &  3 & 385\,516.653 & 0.080 \cr
 5 &  4 &  5 &  4 &  3 &  4 & 385\,516.689 & 0.106 \cr
 5 &  5 &  5 &  4 &  4 &  4 & 385\,516.733 & 0.102 \cr
 5 &  5 &  4 &  4 &  4 &  3 & 385\,516.741 & 0.083 \cr
 5 &  5 &  6 &  4 &  4 &  5 & 385\,516.768 & 0.126 \cr
 5 &  6 &  5 &  4 &  5 &  4 & 385\,516.772 & 0.107 \cr
 5 &  6 &  6 &  4 &  5 &  5 & 385\,516.779 & 0.128 \cr
 5 &  6 &  7 &  4 &  5 &  6 & 385\,516.800 & 0.152 \cr
  \multicolumn{8}{c}{$\Delta F=0$}\cr
 5 &  5 &  4 &  4 &  5 &  4 & 385\,514.735 & 0.004 \cr
 5 &  5 &  6 &  4 &  5 &  6 & 385\,514.757 & 0.006 \cr
 5 &  5 &  5 &  4 &  5 &  5 & 385\,514.764 & 0.003 \cr
 5 &  4 &  4 &  4 &  3 &  4 & 385\,516.224 & 0.005 \cr
 5 &  5 &  5 &  4 &  4 &  5 & 385\,516.309 & 0.005 \cr
 5 &  6 &  6 &  4 &  5 &  6 & 385\,516.314 & 0.003 \cr
 5 &  4 &  3 &  4 &  3 &  3 & 385\,517.154 & 0.006 \cr
 5 &  5 &  4 &  4 &  4 &  4 & 385\,517.207 & 0.003 \cr
 5 &  6 &  5 &  4 &  5 &  5 & 385\,517.275 & 0.004 \cr
 5 &  4 &  4 &  4 &  4 &  4 & 385\,519.050 & 0.005 \cr
 5 &  4 &  3 &  4 &  4 &  3 & 385\,519.086 & 0.003 \cr
 5 &  4 &  5 &  4 &  4 &  5 & 385\,519.091 & 0.005 \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
\end{tabular}
\begin{list}{}{}
\item[$^{\mathrm{a}}$] the estimated uncertainty based on propagation of the  spectroscopic constants' errors
is 10 kHz
\end{list}
\end{table}

\begin{table}[htbp]
 \caption{Calculated hyperfine components (MHz)$^{\mathrm{a}}$ and relative intensities of the $J=6 \leftarrow 5$
 transition of N$_2$D$^+$}\label{list5}
 \centering
 \begin{tabular}{ccccccD{.}{.}{3}D{.}{.}{3}}

 \hline \noalign{\smallskip}
  $J'$ & $F_1'$ & $F'$ & $J$ & $F_1$ & $F$ & \multicolumn{1}{c}{Calc. Freq.} & \multicolumn{1}{c}{Rel. Int.} \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
  \multicolumn{8}{c}{$\Delta F=+1$}\cr
 6 &  5 &  4 &  5 &  4 &  3 & 462\,603.777 & 0.071 \cr
 6 &  5 &  5 &  5 &  4 &  4 & 462\,603.785 & 0.087 \cr
 6 &  5 &  6 &  5 &  4 &  5 & 462\,603.809 & 0.108 \cr
 6 &  6 &  6 &  5 &  5 &  5 & 462\,603.839 & 0.105 \cr
 6 &  6 &  5 &  5 &  5 &  4 & 462\,603.839 & 0.089 \cr
 6 &  6 &  7 &  5 &  5 &  6 & 462\,603.863 & 0.124 \cr
 6 &  7 &  6 &  5 &  6 &  5 & 462\,603.866 & 0.108 \cr
 6 &  7 &  7 &  5 &  6 &  6 & 462\,603.874 & 0.126 \cr
 6 &  7 &  8 &  5 &  6 &  7 & 462\,603.890 & 0.145 \cr
  \multicolumn{8}{c}{$\Delta F=0$}\cr
 6 &  6 &  5 &  5 &  6 &  5 & 462\,601.801 & 0.003 \cr
 6 &  6 &  7 &  5 &  6 &  7 & 462\,601.819 & 0.004 \cr
 6 &  6 &  6 &  5 &  6 &  6 & 462\,601.823 & 0.002 \cr
 6 &  5 &  5 &  5 &  4 &  5 & 462\,603.320 & 0.003 \cr
 6 &  6 &  6 &  5 &  5 &  6 & 462\,603.380 & 0.003 \cr
 6 &  7 &  7 &  5 &  6 &  7 & 462\,603.387 & 0.002 \cr
 6 &  5 &  4 &  5 &  4 &  4 & 462\,604.278 & 0.004 \cr
 6 &  6 &  5 &  5 &  5 &  5 & 462\,604.312 & 0.003 \cr
 6 &  7 &  6 &  5 &  6 &  6 & 462\,604.361 & 0.003 \cr
 6 &  5 &  5 &  5 &  5 &  5 & 462\,606.102 & 0.003 \cr
 6 &  5 &  4 &  5 &  5 &  4 & 462\,606.122 & 0.002 \cr
 6 &  5 &  6 &  5 &  5 &  6 & 462\,606.132 & 0.003 \cr
 \noalign{\smallskip} \hline \noalign{\smallskip}
\end{tabular}
\begin{list}{}{}
\item[$^{\mathrm{a}}$] the estimated uncertainty based on propagation of the  spectroscopic constants' errors
is 16 kHz
\end{list}
\end{table}

\end{document}
