\begin{table}%t7
\caption{\label{tabn2hp65}Hyperfine components and $A_{ul}$ Einstein spontaneous emission coefficients of the \jscb transition of N$_2$H$^+$.}
\small%\centerline
 {
 \begin{tabular}{cccccccc}
 \hline\hline
  $J'$ & $F_1'$ &  \multicolumn{2}{c}{$F' \rightarrow J$}  & $F_1$ & $F$ & \multicolumn{1}{c}{Frequency$^{{a}}$} & \multicolumn{1}{c}{$A_{ul}$} \cr
  &&&&&& \multicolumn{1}{c}{(MHz)}& \multicolumn{1}{c}{(s$^{-1}$)}\cr
 \hline
6&6&6&5&6&7&558~963.91& $7.094(-6)$\\
6&6&6&5&6&5&558~963.93& $7.081(-6)$\\
6&6&5&5&6&5&558~964.39& $2.929(-4)$\\
6&6&7&5&6&7&558~964.41& $2.951(-4)$\\
6&6&6&5&6&6&558~964.42& $2.871(-4)$\\
6&6&5&5&6&6&558~964.88& $8.368(-6)$\\
6&6&7&5&6&6&558~964.92& $6.148(-6)$\\
6&5&5&5&4&5&558~965.91& $4.195(-4)$\\
6&6&6&5&5&6&558~965.97& $2.929(-4)$\\
6&7&7&5&6&7&558~965.98& $2.213(-4)$\\
6&5&5&5&6&5&558~966.18& $6.916(-8)$\\
6&5&4&5&4&3&558~966.38& $9.969(-3)$\\
6&5&5&5&4&4&558~966.39& $1.007(-2)$\\
6&5&4&5&4&5&558~966.39& $5.179(-6)$\\
6&5&6&5&4&5&558~966.42& $1.049(-2)$\\
6&6&5&5&5&6&558~966.44& $2.421(-6)$\\
6&6&5&5&5&4&558~966.44& $1.020(-2)$\\
6&6&6&5&5&5&558~966.45& $1.025(-2)$\\
6&7&6&5&6&7&558~966.46& $1.310(-6)$\\
6&6&7&5&5&6&558~966.47& $1.054(-2)$\\
6&7&6&5&6&5&558~966.47& $1.059(-2)$\\
6&7&7&5&6&6&558~966.48& $1.062(-2)$\\
6&7&8&5&6&7&558~966.50& $1.085(-2)$\\
6&5&4&5&6&5&558~966.67& $2.490(-6)$\\
6&5&5&5&6&6&558~966.67& $2.421(-6)$\\
6&5&6&5&6&7&558~966.68& $2.431(-6)$\\
6&5&6&5&6&5&558~966.69& $4.092e{-}10$\\
6&5&4&5&4&4&558~966.88& $5.127(-4)$\\
6&6&5&5&5&5&558~966.91& $3.462(-4)$\\
6&7&6&5&6&6&558~966.96& $2.554(-4)$\\
6&5&6&5&6&6&558~967.18& $5.852(-8)$\\
6&5&5&5&5&6&558~968.27& $1.169(-5)$\\
6&5&5&5&5&4&558~968.23& $1.165(-5)$\\
6&5&5&5&5&5&558~968.70& $3.327(-4)$\\
6&5&4&5&5&4&558~968.72& $3.418(-4)$\\
6&5&6&5&5&6&558~968.74& $3.462(-4)$\\
6&5&4&5&5&5&558~969.19& $1.424(-5)$\\
6&5&6&5&5&5&558~969.21& $9.890(-6)$\\
 \hline
\end{tabular}}
\medskip
$^{{a}}$ The frequency uncertainty is $\pm$0.18 MHz for all hyperfine \mbox{components}. 
\end{table}