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Table 3

Effective spectroscopic constants determined from state-by-state fits of the rotational transitions measured for the ground and v4 = 1, v5 = 1, v4 = v5 = 1 states of 12C2HDa.

Parameter Unit G . S . v4 = 1 v5 = 1 v4 = v5 = 1

B MHz 29725.24646(27) 29805.44743(32) 29770.36999(18) 29849.79104(50)
Previous value 29725.24501(82)b 29803.0066(43)c 29766.7458(44)c
D kHz 34.0383(41) 35.1929(21) 34.5408(10) 35.5450(43)
Previous value 34.0186(45)b 35.107(44)c 34.482(54)c
H Hz 0.090(18)
γ 44 MHz –2.44328d –2.44328d
δ 44 kHz –0.1003 d
γ 55 MHz –3.62753d –3.62753d
δ 55 kHz –0.0767 d
γ 45 MHz 0.07645(52)
q t MHz 133.05208(66) 105.69975(36) e
Previous value 133.0259(71)c 105.6843(65)c
kHz –1.1512(42) -0.6544(21) f
Previous value –1.205(26)c –0.693(24)c
g 45 GHz 20.9453(26)
r 45 GHz 64.5713(27)
MHz –0.72846(35)
σ fit kHz 2.9 7.5 4.4 12.5
No. of lines 10 17 18 25
J range 1–10 1–10 1–10 1–8

Notes.

(a)

Estimated uncertainties (1σ) are given in parentheses in units of the last figure quoted.

(d)

Fixed in the analysis at the value extrapolated from the doubly and triply excited bending states.

(e)

q4 and q5 fixed in the analysis at the values determined for the singly excited bending states.

(f)

and fixed in the analysis at the values determined for the singly excited bending states.

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