Table 8: FIR line ratios after correcting the observed [C II] intensities for emission from the ionized medium. We study two cases: the emission of [C II] from the ionized medium originates entirely a) from the diffuse medium, and b), that the emission arises entirely from dense H II regions. Also shown is the intensity ratio $\epsilon $ of the two major cooling lines of PDRs ([O I](63)+[C II] $_{\rm PDR}$) vs. the observed TIR continuum.
$\Delta\alpha/\Delta\delta$ [C II] $_{\rm obs}$   [C II] $_{\rm PDR}$   [O I](63) $\epsilon $
  [N II](122)   [C II] $_{\rm obs}$   [C II] $_{\rm PDR}$ [%]
a) [N II] only from the DIM:    
M 83:            
0, 0 5.8   0.02   57.41 0.12
-80,-72 7.3   0.22   3.18 0.22
89, 38 5.7   0.00   - 0.17
M 51:            
0, 0 3.6   0.00   - 0.08
72, 84 7.3   0.22   3.59 0.16
-84,-84 7.4   0.23   3.78 0.21
b) [N II] only from H II-regions:    
M 83:            
0, 0 5.8   0.81   1.31 0.21
-80,-72 7.3   0.85   0.83 0.36
89, 38 5.7   0.81   0.99 0.35
M 51:            
0, 0 3.6   0.69   1.06 0.16
72, 84 7.3   0.85   0.91 0.25
-84,-84 7.4   0.85   1.02 0.33


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