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Table A.1.
Zeeman parameters, frequencies, and Einstein coefficients of CN transitions that are relevant to ALMA polarisation measurements.
| N | J | F | N′ | J′ | F′ | ν (GHz)a | z (Hz/μG) | A × 106 (s−1)a |
|---|---|---|---|---|---|---|---|---|
| 1 | 1/2 | 1/2 | 0 | 1/2 | 1/2 | 113.1233701(58) | −0.62 | 1.29 |
| 1 | 1/2 | 1/2 | 0 | 1/2 | 3/2 | 113.1441573(57) | 2.18 | 10.53 |
| 1 | 1/2 | 3/2 | 0 | 1/2 | 1/2 | 113.1704915(39) | −0.3 | 5.14 |
| 1 | 1/2 | 3/2 | 0 | 1/2 | 3/2 | 113.1912787(34) | 0.63 | 6.68 |
| 1 | 3/2 | 3/2 | 0 | 1/2 | 1/2 | 113.4881202(33) | 2.17 | 6.74 |
| 1 | 3/2 | 5/2 | 0 | 1/2 | 3/2 | 113.4909702(24) | 0.56 | 11.92 |
| 1 | 3/2 | 1/2 | 0 | 1/2 | 1/2 | 113.4996443(28) | 0.62 | 10.63 |
| 1 | 3/2 | 3/2 | 0 | 1/2 | 3/2 | 113.5089074(28) | 1.62 | 5.19 |
| 1 | 3/2 | 1/2 | 0 | 1/2 | 3/2 | 113.5204315(44) | 1.56 | 1.30 |
| 2 | 3/2 | 1/2 | 1 | 3/2 | 1/2 | 226.2874185(69) | 0.62 | 10.30 |
| 2 | 3/2 | 1/2 | 1 | 3/2 | 3/2 | 226.2989427(68) | 2.17 | 8.23 |
| 2 | 3/2 | 3/2 | 1 | 3/2 | 1/2 | 226.3030372(64) | −1.8 | 4.17 |
| 2 | 3/2 | 3/2 | 1 | 3/2 | 3/2 | 226.3145400(500) | 0.27 | 9.90 |
| 2 | 3/2 | 3/2 | 1 | 3/2 | 5/2 | 226.3324986(56) | 2.58 | 4.56 |
| 2 | 3/2 | 5/2 | 1 | 3/2 | 3/2 | 226.3419298(54) | −2.2 | 3.16 |
| 2 | 3/2 | 5/2 | 1 | 3/2 | 5/2 | 226.3598710(500) | 0.22 | 16.08 |
| 2 | 3/2 | 1/2 | 1 | 1/2 | 3/2 | 226.6165714(53) | −0.3 | 10.73 |
| 2 | 3/2 | 3/2 | 1 | 1/2 | 3/2 | 226.6321901(35) | −0.72 | 42.59 |
| 2 | 3/2 | 5/2 | 1 | 1/2 | 3/2 | 226.6595584(26) | −0.71 | 94.67 |
| 2 | 3/2 | 1/2 | 1 | 1/2 | 1/2 | 226.6636928(25) | −0.62 | 84.65 |
| 2 | 3/2 | 3/2 | 1 | 1/2 | 1/2 | 226.6793114(31) | −1.18 | 52.68 |
| 2 | 5/2 | 5/2 | 1 | 3/2 | 3/2 | 226.8741908(23) | 0.71 | 96.22 |
| 2 | 5/2 | 7/2 | 1 | 3/2 | 5/2 | 226.8747813(30) | 0.4 | 114.32 |
| 2 | 5/2 | 3/2 | 1 | 3/2 | 1/2 | 226.8758960(20) | 1.18 | 85.87 |
| 2 | 5/2 | 3/2 | 1 | 3/2 | 3/2 | 226.8874202(29) | 1.47 | 27.31 |
| 2 | 5/2 | 5/2 | 1 | 3/2 | 5/2 | 226.8921280(27) | 1.06 | 18.10 |
| 2 | 5/2 | 3/2 | 1 | 3/2 | 5/2 | 226.9053574(44) | 0.79 | 1.13 |
| 2 | 5/2 | 5/2 | 1 | 1/2 | 3/2 | 227.1918195(49) | 2.2 | 0.0015 |
| 3 | 5/2 | 3/2 | 2 | 5/2 | 3/2 | 339.4467770(500) | 0.22 | 22.64 |
| 3 | 5/2 | 3/2 | 2 | 5/2 | 5/2 | 339.4599960(70) | 2.57 | 4.33 |
| 3 | 5/2 | 5/2 | 2 | 5/2 | 3/2 | 339.4626359(67) | −2.42 | 2.95 |
| 3 | 5/2 | 5/2 | 2 | 5/2 | 5/2 | 339.4759040(500) | 0.14 | 21.24 |
| 3 | 5/2 | 5/2 | 2 | 5/2 | 7/2 | 339.4932119(70) | 2.69 | 2.99 |
| 3 | 5/2 | 7/2 | 2 | 5/2 | 5/2 | 339.4992884(70) | −2.52 | 2.33 |
| 3 | 5/2 | 7/2 | 2 | 5/2 | 7/2 | 339.5166351(66) | 0.11 | 25.35 |
| 3 | 5/2 | 3/2 | 2 | 3/2 | 5/2 | 339.9922571(56) | −0.33 | 3.89 |
| 3 | 5/2 | 5/2 | 2 | 3/2 | 5/2 | 340.0081263(38) | −0.69 | 61.97 |
| 3 | 5/2 | 3/2 | 2 | 3/2 | 3/2 | 340.0196255(36) | −0.97 | 92.70 |
| 3 | 5/2 | 7/2 | 2 | 3/2 | 5/2 | 340.0315494(34) | −0.45 | 384.49 |
| 3 | 5/2 | 3/2 | 2 | 3/2 | 1/2 | 340.0354080(500) | −0.93 | 288.68 |
| 3 | 5/2 | 5/2 | 2 | 3/2 | 3/2 | 340.0354080(500) | −0.62 | 323.09 |
| 3 | 7/2 | 7/2 | 2 | 5/2 | 5/2 | 340.2477700(500) | 0.45 | 379.66 |
| 3 | 7/2 | 9/2 | 2 | 5/2 | 7/2 | 340.2477700(500) | 0.31 | 413.13 |
| 3 | 7/2 | 5/2 | 2 | 5/2 | 3/2 | 340.2485440(36) | 0.62 | 367.40 |
| 3 | 7/2 | 5/2 | 2 | 5/2 | 5/2 | 340.2617734(37) | 1.01 | 44.79 |
| 3 | 7/2 | 7/2 | 2 | 5/2 | 7/2 | 340.2649490(37) | 0.77 | 33.50 |
| 3 | 7/2 | 5/2 | 2 | 5/2 | 7/2 | 340.2791201(54) | 0.51 | 0.93 |
Notes.
(a)
Line frequencies (with last-digit uncertainties between brackets) and Einstein coefficients were taken from the fits presented in the CDMS database (Müller et al. 2001).
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