Table 4: NGC 1365 line parameters.

Transition		 Gaussian V $T_{\rm A}^{*}$ $\Delta V$
  Component [ ${\rm km~s}^{-1}$] [mK] [ ${\rm km~s}^{-1}$]

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
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 130a
CN 2-1 1 1526 $\pm$ 11 10.4 $\pm$ 1.5 130a
  2 1727 $\pm$ 35 8.4 $\pm$ 1.9 212b
  3 1846 $\pm$ 35 4.11 $\pm$ 3.5 130a
HCN 3-2 1 1534 $\pm$ 5 51.4 $\pm$ 3.4 136 $\pm$ 13
  2 1706 $\pm$ 25 11.4 $\pm$ 3.3 142c
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
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.
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.
c
The second component of HCN 3-2 seems to be affected by noise, so its line width was locked at $\Delta V = 142$  ${\rm km~s}^{-1}$, i.e., the corresponding line width of the CO 1-0 line.

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