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Table 3
Components with weak CO emission toward the continuum target.
| Target | V | τ(1−0) |
|
dN(CO)/dV | Texc(1−0) | p(H2) | n(H2)a | ∫τ(HCO+)dv/total |
| km s-1 | K | 1015 cm-2 (km s-1)-1 | K | 103 cm-3 K | cm-3 | |||
|
|
||||||||
| B0212 | –10.3 | 0.49 | 0.40 | 0.65 | 3.4–3.6 | 1.9–2.5 | 75–100 | 0.122 |
| –0.05 | 0.95 | <0.14b | 1.11 | <3.1–3.2 | <0.9–1.1 | <35–45 | 0.102 | |
| B0224 | –10.6 | 0.43 | <0.10 | 0.48 | <3.0–3.1 | <0.8–1.0 | <30–40 | 0.161 |
| B0355 | –13.9 | 0.45 | 0.31 | 0.52 | 3.8–4.0 | 3.0–3.5 | 120–140 | 0.224 |
| –4.0 | 0.86 | 0.37 | 1.10 | 3.6–3.8 | 2.1–2.5 | 85–100 | 0.204 | |
| B0528 | 2.8 | <0.11 | <0.16 | 0.080 | ||||
| B1730 | 5.1 | 1.15 | 0.24 | 1.42 | 3.5–3.7 | 1.8–2.2 | 70–90 | 1.000 |
| B1928 | −3 | <0.11 | <0.11 | 1.000 | ||||
Notes. Using CO parameters originally derived by Liszt & Lucas (1998) and τ(HCO + ) from Lucas & Liszt (1996); ;
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