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Table 8:

Lower state quantum numbers of rotational transitions of 13CH313CN, frequencies (MHz), uncertainties unc. (kHz), and residuals o-c (kHz) between observed frequencies and those calculated from the final set of spectroscopic parameters.
J'' K'' Frequency unc. o-c J'' K'' Frequency unc. o-c J'' K'' Frequency unc. o-c
13 4 249849.289 30 30 18 5 338978.878 50 2 51 2 926328.788 200 -108
13 3 249881.971 10 -5 18 2 339111.819 15 -6 51 1 926379.428 200 -194
14 4 267689.340 20 -8 25 3 463885.870 50 22 54 3 979425.780 150 20
14 3 267724.401 10 9 25 2 463929.028 50 -11 60 6 1085127.880 150 34
14 2 267749.425 10 -7 27 3 499525.679 100 88 60 4 1085519.654 150 -68
14 1 267764.473 15 12 34 7 623721.761 200 -22 60 3 1085656.847 200 -150
15 6 285421.490 40 21 34 5 623998.639 150 -25 60 0 1085833.407 200 -177
15 4 285528.155 30 18 34 4 624102.519 150 -85 61 9 1101913.821 100 -11
15 3 285565.500 15 -4 34 3 624183.422 100 -68 61 5 1103025.791 150 69
15 2 285592.188 15 -17 34 2 624241.332 50 45 61 4 1103204.664 150 -125
15 1 285608.237 30 7 35 9 641127.171 200 161 61 2 1103443.760 150 55
16 6 303252.220 25 -24 35 3 641980.261 80 -29 61 1 1103503.550 150 88
16 1 303450.598 15 -8 35 1 642075.314 80 -31 62 6 1120480.948 200 154
17 6 321081.547 15 -6 50 3 908507.997 150 -88 62 4 1120884.433 200 -34
17 5 321147.495 20 9 50 2 908591.195 150 123 62 3 1121025.872 100 -3
17 4 321201.474 15 8 50 0 908657.612 150 132 62 2 1121126.880 150 -39
17 3 321243.472 5 -0 51 6 925788.347 200 -80 63 2 1138804.705 200 60
17 2 321273.504 10 15 51 3 926244.313 200 -61 63 1 1138866.331 200 163
17 1 321291.490 15 -13                    


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