Table 4
Properties of the ionized gas derived from its thermal emission.
θ | ℒ a | EM b | ⟨ ne ⟩ c | ⟨ Ne ⟩ d | ![]() |
![]() |
(″) | pc | pc cm-6 | cm-4 | cm-2 | K km s-1 | K km s-1 |
|
||||||
21.3 | 269 | 1.7 × 104 | 8 | 6.59 × 1021 | 758 | 85.8 |
18 | 227 | 2.4 × 104 | 10 | 7.17 × 1021 | 856 | 113 |
14 | 177 | 3.9 × 104 | 15 | 8.13 × 1021 | 1013 | 100 |
2 | 25.2 | 1.9 × 106 | 280 | 2.15 × 1022 | 60.1 | 9.5 |
1.7 | 21.4 | 2.7 × 106 | 350 | 2.33 × 1022 | 47.1 | 7.3 |
1.61f | 20.3 | 42.3 | 6.5 | |||
1.55g | 19.5 | 39.2 | 6.0 | |||
1 | 12.6 | 7.7 × 106 | 780 | 3.04 × 1022 | 21.3 | 3.0 |
Notes. Boldfaced numbers are the expected intensities when accounting for the frequency dependent coupling of the compact H II regions to the SOFIA beam.
Integrated [C II] and [N II] intensity assuming Te = 8000 K and an electron density of ⟨ ne ⟩ for collisional excitation. The intensity is corrected by the area filling factors min(1,θ2/ 142) and min(1,θ2/ 182) for the [C II] and [N II] beams, respectively.
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