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Table 2

Measured frequencies of the 21,1 − 20,2 transition, and residuals from the global fit of the Infrared, and submillimeter-wave data for 15NH2.

Upper level Lower level Frequency(Unc.) O.C.
N ′′ J ′′ a a F ′′ a N J a a F a (in MHz) (in MHz)

2 1 1 3 3 1 4 2 0 2 2 2 1 3 639 001.675(0.100) 0.01381
2 1 1 3 2 1 3 2 0 2 2 2 1 2 639 045.833(0.100) –0.01377
2 1 1 3 3 1 3 2 0 2 2 2 1 3 639 051.520(0.100) –0.06082
2 1 1 3 2 1 3 2 0 2 2 1 1 2 639 076.520(0.100) 0.15477
2 1 1 3 3 1 3 2 0 2 2 2 1 2 639 083.185(0.100) –0.05989
2 1 1 3 2 1 3 2 0 2 3 2 1 2 640 725.613(0.100) 0.01293
2 1 1 3 2 1 3 2 0 2 3 3 1 2 640 744.982(0.100) 0.05757
2 1 1 3 2 1 2 2 0 2 3 2 1 1 640 746.216(0.100) –0.00670
2 1 1 3 3 1 4 2 0 2 3 3 1 3 640 754.822(0.100) –0.09119
2 1 1 3 3 1 3 2 0 2 3 2 1 2 640 763.042(0.100) 0.04531
2 1 1 3 2 1 3 2 0 2 3 3 1 3 640 767.442(0.100) 0.00550
2 1 1 3 3 1 2 2 0 2 3 2 1 1 640 770.846(0.100) 0.02358
2 1 1 3 2 1 2 2 0 2 3 2 1 2 640 774.637(0.100) 0.20803
2 1 1 3 2 1 1 2 0 2 3 2 1 1 640 783.056(0.100) –0.02160
2 1 1 3 2 1 3 2 0 2 3 2 1 3 640 788.517(0.100) –0.06519
2 1 1 3 2 1 2 2 0 2 3 3 1 2 640 793.745(0.100) –0.00903
2 1 1 3 3 1 2 2 0 2 3 2 1 2 640 799.061(0.100) 0.03280
2 1 1 3 3 1 3 2 0 2 3 3 1 3 640 804.861(0.100) 0.02749
2 1 1 3 3 1 4 2 0 2 3 3 1 4 640 809.536(0.100) 0.00173
2 1 1 3 2 1 2 2 0 2 3 3 1 3 640 816.075(0.100) –0.19030
2 1 1 3 3 1 2 2 0 2 3 3 1 2 640 818.465(0.100) 0.11185
2 1 1 3 3 1 3 2 0 2 3 2 1 3 640 825.896(0.100) –0.08381
2 1 1 3 2 1 2 2 0 2 3 2 1 3 640 837.348(0.100) –0.06369
2 1 1 3 3 1 2 2 0 2 3 3 1 3 640 840.873(0.100) 0.00808
2 1 1 3 3 1 3 2 0 2 3 3 1 4 640 859.407(0.100) –0.04760
2 1 1 2 2 1 2 2 0 2 2 2 1 3 645 111.178(0.100) –0.07048
2 1 1 2 2 1 1 2 0 2 2 2 1 2 645 118.784(0.100) –0.03407
2 1 1 2 2 1 2 2 0 2 2 2 1 2 645 142.843(0.100) –0.06885
2 1 1 2 2 1 1 2 0 2 2 2 1 1 645 148.420(0.100) –0.19977
2 1 1 2 2 1 3 2 0 2 2 2 1 3 645 150.805(0.100) –0.06829
2 1 1 2 1 1 2 2 0 2 2 2 1 3 645 159.555(0.100) –0.11288
2 1 1 2 2 1 2 2 0 2 2 2 1 1 645 173.299(0.100) 0.38419
2 1 1 2 2 1 2 2 0 2 2 1 1 2 645 173.299(0.100) 0.38419
2 1 1 2 1 1 1 2 0 2 2 2 1 1 645 180.728(0.100) 0.06478
2 1 1 2 1 1 1 2 0 2 2 1 1 2 645 180.728(0.100) 0.06478
2 1 1 2 1 1 2 2 0 2 2 2 1 2 645 191.191(0.100) –0.14075
2 1 1 2 1 1 0 2 0 2 2 1 1 1 645 196.231(0.100) –0.04154
2 1 1 2 2 1 1 2 0 2 2 1 1 0 645 206.745(0.100) –0.05118
2 1 1 2 2 1 2 2 0 2 2 1 1 1 645 211.750(0.100) 0.00473
2 1 1 2 2 1 3 2 0 2 2 1 1 2 645 213.055(0.100) 0.00028
2 1 1 2 1 1 1 2 0 2 2 1 1 1 645 219.340(0.100) –0.02789
2 1 1 2 1 1 2 2 0 2 2 2 1 1 645 221.750(0.100) 0.51794
2 1 1 2 1 1 2 2 0 2 2 1 1 2 645 221.750(0.100) 0.51794
2 1 1 2 1 1 1 2 0 2 2 1 1 0 645 238.429(0.100) –0.08367
2 1 1 2 1 1 2 2 0 2 2 1 1 1 645 260.088(0.100) –0.07677
2 1 1 2 2 1 1 2 0 2 3 3 1 2 646 818.042(0.100) 0.14697
2 1 1 2 2 1 2 2 0 2 3 3 1 3 646 864.569(0.100) 0.06762
2 1 1 2 2 1 2 2 0 2 3 2 1 3 646 885.610(0.100) –0.03728
2 1 1 2 1 1 2 2 0 2 3 2 1 3 646 933.946(0.100) –0.12137
2 1 1 2 2 1 3 2 0 2 3 3 1 4 646 958.718(0.100) –0.02867

Notes. The complete version of the fit including all the measurements is available at the CDS: S1.

(a)

Following SPFIT format half-integer spins are rounded up to the next integer.

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