Table 8.

Calculated and experimental (Ulenikov et al. 2002) k = 7 and k = 8, A1 − A2 splittings (in MHz) and their sensitivities in the ν3 vibrational state of PH3.

JνexpνcalcTνexpνcalcT
k = 7k = 8
1230.55−641340743.7−91
1312601701.441821034
14181787660.21313610565−4.91
152585.527.61344.4−22.3
16807.4−1.111370.211.7
171485.1−22.95056.4−16.8
181315.0−41773.0−3.1
JνexpνcalcTνexpνcalcT
k = 7k = 8
1230.55−641340743.7−91
1312601701.441821034
14181787660.21313610565−4.91
152585.527.61344.4−22.3
16807.4−1.111370.211.7
171485.1−22.95056.4−16.8
181315.0−41773.0−3.1
Table 8.

Calculated and experimental (Ulenikov et al. 2002) k = 7 and k = 8, A1 − A2 splittings (in MHz) and their sensitivities in the ν3 vibrational state of PH3.

JνexpνcalcTνexpνcalcT
k = 7k = 8
1230.55−641340743.7−91
1312601701.441821034
14181787660.21313610565−4.91
152585.527.61344.4−22.3
16807.4−1.111370.211.7
171485.1−22.95056.4−16.8
181315.0−41773.0−3.1
JνexpνcalcTνexpνcalcT
k = 7k = 8
1230.55−641340743.7−91
1312601701.441821034
14181787660.21313610565−4.91
152585.527.61344.4−22.3
16807.4−1.111370.211.7
171485.1−22.95056.4−16.8
181315.0−41773.0−3.1
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