\begin{table}%t4
      \caption{NGC~1365 line parameters.}
         \label{tab:1365-intensities}
\small
%\centerline
{
         \begin{tabular}{lcccc}
            \hline\hline
            \noalign{\smallskip}
            Transition & Gaussian  & $V$ & $T_{\rm A}^{*}$ & $\Delta V$ \\
                       & Component & [\kms] & [mK] & [\kms] \\
            \noalign{\smallskip}
            \hline
            \noalign{\smallskip}
		CO~1--0 & 1 & 1532~$\pm$~2 & 322.7~$\pm$~5.2 & 136~$\pm$~4\\
		       & 2 & 1709~$\pm$~3 & 260.3~$\pm$~5.0 & 142~$\pm$~5\\
            \noalign{}\\
		CN 1--0 & 1 & 1511~$\pm$~13   & 16.8~$\pm$~3.5 & 130~$\pm$~25\\
		       & 2 & 1685~$\pm$~33   & 8.9~$\pm$~1.4  & 212~$\pm$~92\\
		       & 3 & 2356~$\pm$~18   & 4.7~$\pm$~1.2  & 130$^{a}$\\		   
            \noalign{}\\
		CN 2--1 & 1 & 1526~$\pm$~11 &  10.4~$\pm$~1.5  & 130$^{a}$\\
		       & 2 & 1727~$\pm$~35     &  8.4~$\pm$~1.9 & 212$^{b}$\\
		       & 3 & 1846~$\pm$~35     &  4.11~$\pm$~3.5 & 130$^{a}$\\
            \noalign{}\\            
		HCN 3--2 & 1 & 1534~$\pm$~5 & 51.4~$\pm$~3.4 & 136~$\pm$~13\\
		        & 2 & 1706~$\pm$~25  & 11.4~$\pm$~3.3 & 142$^{c}$\\
            \noalign{}\\
		HNC 1--0 & 1 & 1539~$\pm$~11 & 16.0~$\pm$~1.7 & 142~$\pm$~23\\
		        & 2 & 1750~$\pm$~34 & 5.1~$\pm$~1.4 & 195~$\pm$~98\\
            \noalign{\smallskip}
            \hline
         \end{tabular}}
          \smallskip
\begin{list}{}{}
\item[$^{{a}}$] The two spingroups are supposed to have the same line width, so these were set according to the value found for the main spingroup of the CN~1$-$0 line.
\item[$^{{b}}$] The line width of the second component of the double peak structure was set to the corresponding value found in the CN~1$-$0 line.
\item[$^{{c}}$] The second component of HCN 3--2 seems to be affected by noise, so its line width was locked at $\Delta V = 142$~\kms, i.e., the corresponding line width of the CO~1$-$0 line.
\end{list}     
   \end{table}