Table 3
Radial position of the peak of the integrated intensity profiles, and radii enclosing 68 and 90% of the total flux.
Transition(a) | Rpeak (b) [″] | R68 [″] | R90 [″] |
---|---|---|---|
12CO (2–1) | 0.43 ± 0.02 | 1.38 | 1.81 |
13CO (2–1) | 0.54 ± 0.04 | 1.11 | 1.49 |
C18O (2–1) | 0.63 ± 0.01 | 0.96 | 1.34 |
H2CO (30,3−20,2) | 0.55 ± 0.02 | 1.27 | 1.70 |
H2CO (32,1−22,0) | 0.44 ± 0.15 | − | − |
C2H (37/2−25/2) | 0.51 ± 0.02 | 1.19 | 1.60 |
H13CN (3–2) | 0.48 ± 0.01 | 0.78 | 1.14 |
HC15N (3–2) | 0.60 ± 0.04 | 0.99 | 1.30 |
DCN (3–2) | 0.47 ± 0.02 | 0.99 | 1.43 |
H13CO+ (3–2) | 0.53 ± 0.02 | 0.85 | 1.15 |
CS (5–4) | 0.99 ± 0.01 | 1.22 | 1.55 |
c-C3H2 (244 GHz) | 0.83 ± 0.1(c) | − | − |
c-C3H2 (218 GHz) | 0.0 ± 0.1(c) | − | − |
Continuum 855μm | 0.646 ± 0.002 | 0.71 | 0.82 |
Notes. (a)See table 1 for quantum number formatting. (b)Radial position of peaks were obtained from multiple-Gaussian fitting, except for the faint c-C3H2 transitions. (c)Rpeak refers to the peak of the integrated intensity profile, while the uncertainty is assumed to be a quarter of the beam major axis, as Gaussian fitting was not possible.
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