Table 1
Orbital, total orbital, and total atomic angular momentum quantum numbers for the seven CN lines at 113 GHz that provide strong intensities (Crutcher et al. 1999; Falgarone et al. 2008).
| ν0 [GHz] | N′ | J′ | F′ | N′′ | J′′ | F′′ | RI | Z [Hz /μG] | RI·Z |
|
|
|||||||||
| 113.144 | 1 | 1 / 2 | 1 / 2 | 0 | 1 / 2 | 3 / 2 | 8 | 2.18 | 17.4 |
| 113.170 | 1 | 1 / 2 | 3 / 2 | 0 | 1 / 2 | 1 / 2 | 8 | –0.31 | 2.5 |
| 113.191 | 1 | 1 / 2 | 3 / 2 | 0 | 1 / 2 | 3 / 2 | 10 | 0.62 | 6.2 |
| 113.488 | 1 | 3 / 2 | 3 / 2 | 0 | 1 / 2 | 1 / 2 | 10 | 2.18 | 21.8 |
| 113.490 | 1 | 3 / 2 | 5 / 2 | 0 | 1 / 2 | 3 / 2 | 27 | 0.56 | 15.1 |
| 113.499 | 1 | 3 / 2 | 1 / 2 | 0 | 1 / 2 | 1 / 2 | 8 | 0.62 | 5.0 |
| 113.508 | 1 | 3 / 2 | 3 / 2 | 0 | 1 / 2 | 3 / 2 | 8 | 1.62 | 13.0 |
Notes. The last three columns show the relative intensity RI, Zeeman shift Z, and their multiplication for the seven CN lines as presented in Falgarone et al. (2008).
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