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Table 3.

Changes of molecular parameters for the v30 = 1 and 2 vibrational states of g-n-PrCN obtained from our latest fit using Watson’s S reduction compared to the fit of Müller et al. (2016).

Parameters v30 = 1 v30 = 1 v30 = 2 v30 = 2
(MHz) ΔX, (Müller et al. 2016) ΔX, this work ΔΔX, (Müller et al. 2016) ΔΔX, this work
A 58.6419(3) 58.6429(2) 3.7323(5) 3.7305(3)
B −7.93829(5) −7.93825(3) −0.60351(11) −0.60369(6)
C −5.17390(5) −5.17388(3) −0.15973(11) −0.15997(5)
DK × 103 5.005(4) 4.9987(8) 0.782(5) 0.775(2)
DJK × 103 −0.6567(3) −0.6552(2) −0.1385(3) −0.1386(3)
DJ × 106 7.76(4) 7.562(12) 6.36(8) 5.95(2)
d1 × 106 −8.029(10) −8.065(5) −2.455(22) −2.515(8)
d2 × 106 −3.605(3) −3.600(2) −0.280(7) −0.252(5)
HK × 106 0.476(21) 0.3743(13) 0.091(3)
HKJ × 109 −109.5(10) −99.2(4) −20.52(48)
HJK × 109 5.52(8) 5.47(6) 1.548(49)
HJ × 109 −0.0729(23) −0.2193(17)
h1 × 109 −0.148(3) −0.1058(12) −0.159(5) −0.1184(10)
h2 × 1012 −21.98(31) −26.26(67)
h3 × 1012 5.0(5) 13.50(13) 1.15(30)
LJK × 1012 −1.015(98)
LJJK × 1015 20.4(50)
LJ × 1015 −5.299(171)
l1 × 1015 −2.686(98)
χaa −0.061(10) −0.064(10)

WRMS 0.86 1.03
Highest frequency 126597 500128 126475 500060
Max J 65 92 63 87
Max Ka 20 25 19 22
Transitions 906 3538 739 2776

Notes. The molecular parameters of v30 = 1 are expressed as Xv = 1 = Xv = 0 + ΔX and for v30 = 2, they are Xv = 2 = Xv = 0 + 2ΔXv30 = 1 + ΔΔX. Numbers in parantheses represent the uncertainty compared to the last quoted digit. Δχaa in Müller et al. (2016) was fit on the ground-state value from Vormann & Dreizler (1988). Other ground-state parameters used in Müller et al. (2016) were from Belloche et al. (2009). The parameters determined in this work are based on the up-dated ground-state parameters. WRMS was calculated on the fit of all lines including v30 = 1 and 2.

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