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Table B.2

Observed frequencies and fit of CH2DCN in the ground state.

J J′′ Frequency Uncertainty Obs.-Calc.
(MHz) (MHz) (MHz)

28 20 8 27 20 7 482 765.4041e 0.0500
28 20 9 27 20 8 482 765.4041e 0.0500
28 17 11 27 17 10 483 686.7272e 0.0300
28 17 12 27 17 11 483 686.7272e 0.0300
28 16 12 27 16 11 483 953.9374+ 0.0300 –0.0416
28 16 13 27 16 12 483 953.9374+ 0.0300 –0.0416
28 15 13 27 15 12 484 203.4077+ 0.0300 0.0576
28 15 14 27 15 13 484 203.4077+ 0.0300 0.0576
28 14 14 27 14 13 484 435.8082+ 0.0300 –0.0195
28 14 15 27 14 14 484 435.8082+ 0.0300 –0.0195
28 13 15 27 13 14 484 651.8126+ 0.0300 0.0072
28 13 16 27 13 15 484 651.8126+ 0.0300 0.0072
28 12 16 27 12 15 484 851.5592+ 0.0300 –0.0161
28 12 17 27 12 16 484 851.5592+ 0.0300 –0.0161

Notes.The full Table B.2 is available in electronic form at the CDS. A portion with only the 14 lowest frequency transitions is shown here for guidance regarding its form and content. Transitions are assigned with the rotational quantum numbers of the upper (first) and lower (second) levels. Observed frequencies are given. A “b” (seen in the full table) shows the b-type transitions. Transitions without “b” are of a-type. Sign “+” shows the blended transitions. An “e” shows the transitions observed but rejected from the fit as described in the text, because of the significant difference between observed and calculated frequencies; the observed minus calculated difference (Obs.-Calc.) is not given for these transitions.

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