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Table 5
Zeeman splittings for selected thermal transitions of SO, CN, OH, and CCH.
| Molecule | Transition | Frequency | Zeeman splittinga | ||
| (GHz) | (2ΔνZ/| B | = 2Z) | ||||
|
|
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| This work | |||||
| SO | N,J = 2, 2 ← 1, 1 | 86.094 | 0.93 | ||
| N,J = 4, 3 ← 3, 2 | 158.972 | 0.81 | |||
| N,J = 7, 6 ← 6, 6 | 174.929 | 0.65b | |||
| N,J = 4, 5 ← 3, 4 | 178.605 | 0.33b | |||
| N,J = 1, 1 ← 0, 1 | 286.340 | 1.74 | |||
| N,J = 2, 2 ← 1, 2 | 309.502 | 1.21 | |||
| N,J = 2, 1 ← 1, 0 | 329.385 | 1.06 | |||
| N,J = 8, 7 ← 7, 6 | 340.714 | 0.23b | |||
| N,J = 8, 8 ← 7, 7 | 344.310 | 0.07b | |||
| N,J = 9, 8 ← 8, 7 | 384.527 | 0.20 | |||
| N,J = 9, 10←8, 9 | 389.121 | 0.07 | |||
| Shinnaga & Yamamoto (2000) | |||||
| SO | N,J = 0, 1 ← 1, 0 | 30.002 | 1.74 | ||
| N,J = 1, 2 ← 0, 1 | 62.932 | 1.34 | |||
| N,J = 3, 4 ← 2, 3 | 138.178 | 0.80 | |||
| N,J = 4, 5 ← 3, 4 | 178.605 | 0.63 | |||
| Bel & Leroy (1989) | |||||
| SO | N,J = 0, 1 ← 1, 0 | 30.002 | ≤10-3 | ||
| N,J = 2, 2 ← 1, 1 | 99.300 | 1.0 | |||
| N,J = 3, 4 ← 2, 3 | 138.178 | 0.8 | |||
| N,J = 4, 3 ← 3, 2 | 158.972 | 1.0 | |||
| N,J = 5, 5 ← 4, 4 | 215.221 | ≤10-3 | |||
| N,J = 5, 6 ← 4, 5 | 219.949 | 0.5 | |||
| N,J = 2, 1 ← 1, 2 | 236.452 | 1.7 | |||
| CN | N,J,F = 1, 3/2, 3/2 ← 0, 1/2, 1/2 | 113.488 | 2.2 | ||
| N,J,F = 2, 3/2, 3/2 ← 1, 3/2, 5/2 | 226.333 | 2.6 | |||
| OH | N,p,J,F = 1,–1, 3/2, 1← 1, 1,3/2, 1 | 1.665 | 3.27 | ||
| N,p,J,F = 1,–1, 3/2, 2← 1, 1,3/2, 2 | 1.667 | 1.96 | |||
| Crutcher et al. (1996) | |||||
| CN | N,J,F = 1, 1/2, 1/2 ← 0, 1/2, 3/2 | 113.488 | 2.18 | ||
| N,J,F = 1, 3/2, 3/2 ← 0, 1/2, 1/2 | 113.488 | 2.18 | |||
| Bel & Leroy (1998) | |||||
| CCH | N,J,F = 1, 1/2, 0 ← 0, 1/2, 1 | 87.407 | 2.8 | ||
| N,J,F = 2, 3/2, 1 ← 1, 3/2, 2 | 174.819 | 2.8 | |||
| N,J,F = 3, 5/2, 2 ← 2, 5/2, 3 | 262.223 | 2.8 | |||
| N,J,F = 4, 7/2, 3 ← 3, 7/2, 4 | 349.618 | 2.8 | |||
| N,J,F = 5, 9/2, 4 ← 4, 9/2, 5 | 437.003 | 2.8 | |||
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