Table 86
Parameters of our best-fit model of HC3N toward Sgr B2(M).
| Moleculea | Sizeb | T rot c | N d | C int e | C vib f | C N g | ΔVh | V off i | F j |
| (′′) | (K) | (cm-2) | (km s-1) | ||||||
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) |
|
|
|||||||||
| HC3N | 60 | 60 | 4.50 × 1014 | 1.00 | 1.00 | 1.00 | 14.0 | 0.0 | e |
| 20 | 20 | 2.40 × 1014 | 1.00 | 1.00 | 1.00 | 30.0 | 11.0 | e | |
| 20 | 20 | 2.40 × 1014 | 1.00 | 1.00 | 1.00 | 30.0 | –8.0 | e | |
| HC3N, ν7 = 1 | 1.3 | 200 | 5.07 × 1017 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC3N, ν7 = 2 | 1.3 | 200 | 5.07 × 1017 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC3N, ν6 = 1 | 1.3 | 200 | 6.76 × 1017 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC3N, ν5 = 1/ν7 = 3 | 1.3 | 200 | 1.35 × 1018 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC3N, ν6 = ν7 = 1 | 1.3 | 200 | 1.35 × 1018 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC3N, ν4 = 1 | 1.3 | 200 | 2.54 × 1018 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| H13CCCN | 60 | 60 | 3.40 × 1013 | 1.00 | 1.00 | 1.00 | 14.0 | 0.0 | e |
| 20 | 20 | 1.20 × 1013 | 1.00 | 1.00 | 1.00 | 30.0 | 11.0 | e | |
| 20 | 20 | 1.20 × 1013 | 1.00 | 1.00 | 1.00 | 30.0 | –8.0 | e | |
| HC13CCN | 60 | 60 | 3.40 × 1013 | 1.00 | 1.00 | 1.00 | 14.0 | 0.0 | e |
| 20 | 20 | 1.20 × 1013 | 1.00 | 1.00 | 1.00 | 30.0 | 11.0 | e | |
| 20 | 20 | 1.20 × 1013 | 1.00 | 1.00 | 1.00 | 30.0 | –8.0 | e | |
| HCC13CN | 60 | 60 | 3.40 × 1013 | 1.00 | 1.00 | 1.00 | 14.0 | 0.0 | e |
| 20 | 20 | 1.20 × 1013 | 1.00 | 1.00 | 1.00 | 30.0 | 11.0 | e | |
| 20 | 20 | 1.20 × 1013 | 1.00 | 1.00 | 1.00 | 30.0 | –8.0 | e | |
| H13CCCN, ν7 = 1 | 1.3 | 200 | 2.54 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC13CCN, ν7 = 1 | 1.3 | 200 | 2.54 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HCC13CN, ν7 = 1 | 1.3 | 200 | 2.54 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| H13CCCN, ν7 = 2 | 1.3 | 200 | 2.54 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC13CCN, ν7 = 2 | 1.3 | 200 | 2.54 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HCC13CN, ν7 = 2 | 1.3 | 200 | 2.54 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| H13CCCN, ν6 = 1 | 1.3 | 200 | 4.22 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HC13CCN, ν6 = 1 | 1.3 | 200 | 4.22 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
| HCC13CN, ν6 = 1 | 1.3 | 200 | 4.22 × 1016 | 1.00 | 1.69 | 1.69 | 10.0 | 3.0 | e |
Notes. See notes of Table 62.
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