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Home All issues Volume 506 / No 3 (November II 2009) A&A, 506 3 (2009) 1487-1499 Full HTML
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Table 7:

Quantum numbers of rotational transitions of CH2DCN from present work, frequencies (MHz), uncertainties unc. (kHz), and residuals o-c (kHz) between observed frequencies and those calculated from the final set of spectroscopic parameters.
J', Ka', Kc' - J'', Ka'', Kc''a Frequency unc. o-c J', Ka', Kc' - J'', Ka'', Kc''a Frequency unc. o-c
16, 5, d-15, 5, d 277717.406 15 1 52, 2, 50-51, 2, 49 903537.321 100 79
16, 4, d-15, 4, d 277761.128 8 0 52, 1, 51-51, 1, 50 904004.487 200 -106
16, 1, 15-15, 1, 14 279000.540 8 -4 53, 1, 53-52, 1, 52 913688.193 200 -117
18, 10, d-17, 10, d 312026.460 30 -33 53, 5, d-52, 5, d 918213.532 200 244
18, 9, d-17, 9, d 312124.485 25 -1 53, 2, 51-52, 2, 50 920897.991 200 -104
18, 8, d-17, 8, d 312212.301 20 -22 53, 1, 52-52, 1, 51 921264.278 200 -12
19, 1, 19-18, 1, 18 328415.596 20 -4 57, 0, 57-56, 0, 56 983638.923 200 221
19, 10, d-18, 10, d 329351.951 30 -5 57, 7, d-56, 7, d 986718.597 200 -83
19, 3, 17-18, 3, 16 329864.188 20 -3 57, 6, d-56, 6, d 986958.857 100 25
19, 2, 17-18, 2, 16 330013.795 10 2 57, 5, d-56, 5, d 987192.298 100 -104
28, 2, 26-27, 2, 25 486412.193 50 -14 57, 3, 54-56, 3, 53 988062.351 150 64
28, 6, d-27, 6, d 485722.367 50 55 57, 1, 56-56, 1, 55 990226.073 150 -131
28, 5, d-27, 5, d 485817.005 50 17 59, 0, 59-58, 0, 58 1017787.045 100 -42
28, 2, 27-27, 2, 26 485869.754 50 29 59, 3, 56-58, 3, 55 1022618.283 200 305
28, 4, d-27, 4, d 485902.358 50 2 59, 2, 57-58, 2, 56 1024977.054 200 138
28, 3, 26-27, 3, 25 485983.562 50 -53 60, 1, 60-59, 1, 59 1033530.934 200 -76
28, 3, 25-27, 3, 24 485997.103 50 86 60, 2, 59-59, 2, 58 1038125.138 200 458
28, 8, d-27, 8, d 485492.763 50 21 60, 1, 59-59, 1, 58 1041862.576 200 330
28, 7, d-27, 7, d 485614.775 50 69 60, 2, 58-59, 2, 57 1042306.148 250 -269
28, 10, d-27, 10, d 485203.300 120 -60 63, 1, 63-62, 1, 62 1084807.020 150 -95
28, 9, d-27, 9, d 485355.715 120 -32 63, 0, 63-62, 0, 62 1086011.334 100 -55
28, 1, 27-27, 1, 26 487942.201 80 8 63, 10, d-62, 10, d 1089039.445 200 160
29, 4, d-28, 4, d 503235.929 50 4 63, 9, d-62, 9, d 1089381.592 150 -123
29, 3, 27-28, 3, 26 503321.438 100 -2 63, 2, 62-62, 2, 61 1089618.582 80 11
29, 3, 26-28, 3, 25 503337.368 100 -40 63, 8, d-62, 8, d 1089695.853 200 177
29, 2, 27-28, 2, 26 503793.683 50 -15 63, 7, d-62, 7, d 1089985.064 80 29
30, 8, d-29, 8, d 520124.625 80 0 63, 6, d-62, 6, d 1090257.213 80 -35
30, 6, d-29, 6, d 520371.360 100 -16 63, 5, d-62, 5, d 1090528.555 100 1
30, 3, 28-29, 3, 27 520657.371 100 155 63, 4, 60-62, 4, 59 1090822.850 80 -22
30, 3, 27-29, 3, 26 520676.142 100 14 63, 4, 59-62, 4, 58 1090859.365 120 -65
30, 2, 28-29, 2, 27 521175.868 100 -24 63, 3, 60-62, 3, 59 1091699.685 80 31
31, 1, 31-30, 1, 30 535476.485 100 21 63, 1, 62-62, 1, 61 1093420.205 80 13
36, 1, 36- 35, 1, 35 621614.941 30 -32 64, 10, d-63, 10, d 1106217.421 200 -65
36, 11, d-35, 11, d 623372.367 100 24 64, 7, d-63, 7, d 1107179.127 80 44
36, 0, 36-35, 0, 35 623466.170 70 -63 64, 1, 63-63, 1, 62 1110587.991 120 -91
36, 10, d-35, 10, d 623587.841 50 -40 64, 2, 62-63, 2, 61 1111566.310 200 175
36, 9, d-35, 9, d 623783.719 100 -30 65, 1, 65-64, 1, 64 1118961.766 200 224
36, 7, d-35, 7, d 624118.615 50 30 65, 0, 65-64, 0, 64 1120088.060 200 -151
36, 6, d-35, 6, d 624259.658 70 -55 65, 8, d-64, 8, d 1124068.425 200 150
36, 2, 35-35, 2, 34 624357.951 50 81 65, 6, d-64, 6, d 1124651.425 200 25
36, 5, d-35, 5, d 624386.762 70 -54 65, 4, 62-64, 4, 61 1125246.197 150 32
36, 3, 33-35, 3, 32 624671.021 50 56 65, 3, 62-64, 3, 61 1126225.423 200 210
36, 2, 34-35, 2, 33 625480.300 40 -32 65, 1, 64-64, 1, 63 1127746.725 100 50
37, 1, 37-36, 1, 36 638831.212 30 -51 65, 2, 63-64, 2, 62 1128865.300 120 71
37, 11, d-36, 11, d 640652.376 100 -27 66, 4, 63-65, 4, 62 1142450.318 100 -121
37, 10, d-36, 10, d 640873.836 70 -23 66, 4, 62-65, 4, 61 1142500.850 100 70
37, 9, d-36, 9, d 641075.115 50 -46 66, 3, 64-65, 3, 63 1142588.221 120 13
37, 8, d-36, 8, d 641256.800 50 4 66, 1, 65 - 65, 1, 64 1144895.808 200 -15
37, 5, d-36, 5, d 641696.453 20 3 66, 2, 64-65, 2, 63 1146157.487 50 -17
37, 3, 34-36, 3, 33 641996.762 50 -64 67, 1, 67-66, 1, 66 1153091.574 200 -94
37, 1, 36-36, 1, 35 644319.793 40 -22 67, 10, d-66, 10, d 1157721.118 200 25
51, 1, 51-50, 1, 50 879398.852 150 -74 67, 7, d-66, 7, d 1158730.616 200 138
51, 6, d-50, 6, d 883499.518 100 -149 68, 1, 68-67, 1, 67 1170147.296 150 -169
51, 5, d- 50, 5, d 883699.093 100 25 68, 0, 68-67, 0, 67 1171160.249 80 98
51, 3, 49-50, 3, 48 884076.317 150 -113 68, 8, d-67, 8, d 1175587.939 200 -178
51, 2, 49-50, 2, 48 886173.147 200 119 68, 6, d-67, 6, d 1176204.005 200 -226
52, 1, 52-51, 1, 51 896546.406 150 179 68, 1, 67-67, 1, 66 1179165.037 200 -191
52, 0, 52 - 51, 0, 51 898157.427 150 45 69, 1, 69-68, 1, 68 1187196.902 200 -100
52, 2, 51-51, 2, 50  900538.159b 150 -1 69, 0, 69-68, 0, 68 1188172.743 200 74
52, 7, d-51, 7, d  900538.159b 150 -1 69, 1, 68-68, 1, 67 1196285.083 200 -134

a A ``d'' given for Kc signals that the asymmetry doubling has not been resolved for the respective Ka. The uncertainty and the residual refer to the average. Since J - Ka - Kc = 0 or 1, Kc is redundant in such case.
b Blended lines treated as intensity weighted average in the fit.


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