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Table 5
O i abundance calculations.
| Component | Jet | Bow-shock | outflow cavity | |
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| Low-excitation assumption | N(CO) (1016 cm-2) | 9.0 | – | 70.0 |
| Tkin (K) | 80–100 | – | 55–85 | |
| n (cm-3) | (0.5–1) × 105 | – | (1–8) × 105 | |
| N(O i) (1016 cm-2) | 24.6 ± 8.5 | – | >24.8 | |
| N(O i)/N(CO) | 2.7 ± 0.9 | – | >0.4 | |
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| High-excitation assumption | N(CO) (1016 cm-2) | 1.5 | 10.0 | 6.0 |
| Tkin (K) | 400–750 | 400–500 | 500–1500 | |
| n (cm-3) | (0.5–1) × 106 | (1.0–2.0) × 106 | (1–5) × 106 | |
| N(O i) (1016 cm-2) | 4.0 ± 1.0 | 2.1 ± 0.6 | >4.9 | |
| N(O i)/N(CO) | 2.7 ± 0.6 | 0.2 ± 0.1 | >0.8 | |
Notes. The (N(CO), Tkin, n) values are those determined by L15 for the “low-” or “high”-excitation component of the CO observations (see text). The uncertainty on N(O i) accounts for the uncertainty on the Tex value, integrated intensity value, and filling factor correction.
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