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
of the two major
cooling lines of PDRs ([O I](63)+[C II]
)
vs. the observed TIR
continuum.
 |
[C II]
 |
|
[C II]
 |
|
[O I](63) |
 |
|
[N II](122) |
|
[C II]
 |
|
[C II]
 |
[%] |
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 |
Source LaTeX |
All tables |
In the text