Table B.1.
CN components and their polarisation and magnetic field limits.
| Transition | Fitted frequencya | Catalogue frequencya | Offset | Peak fluxb | mc limitc | |Bz| limitd |
|---|---|---|---|---|---|---|
| (CN N = 2−1) | (GHz) | (GHz) | (MHz) | (mJy beam−1) | (%) | (mG) |
| J = 3/2−3/2, F = 3/2−5/2 | 226.3325190(90) | 226.3324986(56) | +0.020 | 8.9 ± 0.7 | 11.0 | 20.0 |
| J = 3/2−3/2, F = 5/2−3/2 | 226.3419360(90) | 226.3419298(54) | +0.006 | 9.0 ± 0.7 | 11.4 | 24.0 |
| J = 3/2−3/2, F = 5/2−5/2 | 226.3598850(50) | 226.3598710(500) | +0.014 | 41.2 ± 1.3 | 1.92 | 42.0 |
| J = 3/2−1/2, F = 3/2−3/2 | 226.6321980(30) | 226.6321901(35) | +0.008 | 64.2 ± 1.2 | 1.72 | 11.0 |
| J = 3/2−1/2, F = 5/2−3/2 | 226.6595630(30) | 226.6595584(26) | +0.005 | 130.5 ± 2.1 | 0.84 | 5.5 |
| J = 3/2−1/2, F = 1/2−1/2 | 226.6636960(30) | 226.6636928(25) | +0.003 | 64.5 ± 1.5 | 1.58 | 12.6 |
| J = 5/2−3/2, F = 5/2−3/2 | 226.8741880(20) | 226.8741908(23) | −0.001 | 129.2 ± 1.6 | 1.02 | 6.7 |
| J = 5/2−3/2, F = 7/2−5/2 | 226.8747813(20) | 226.8757813(30) | [0] | 157.6 ± 1.6 | 0.84 | 11.2 |
| J = 3/2−3/2, F = 3/2−5/2 | 226.8758960(110) | 226.8758960(20) | 0.000 | 101.8 ± 7.3 | 1.30 | 5.1 |
| J = 3/2−3/2, F = 3/2−5/2 | 226.8874040(40) | 226.8874202(29) | −0.020 | 47.0 ± 1.3 | 2.06 | 7.2 |
| J = 3/2−3/2, F = 3/2−5/2 | 226.8921260(40) | 226.8921280(27) | −0.002 | 46.1 ± 1.2 | 2.39 | 11.0 |
Notes.
The fitted frequency was derived by a fit to our data using the CN N = 2−1, J = 5/2−3/2, F = 7/2−5/2 transition as reference, the catalogue frequency is taken from the CDMS catalogue of Müller et al. (2001). The uncertainty in the last digits is indicated between brackets. The shift between the two is similar to that reported for a subset of transitions in Teague et al. (2016).
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