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Table A.1.

Experimental spectroscopic parameters for the ground vibrational state of maleonitrile

Parameter / Unit This work a This work HFS b Halter et al. (2001)
A / MHz 7389.5215(14) 7389.51061(35) 7389.5090(7)
B / MHz 2672.59327(85) 2672.59436(11) 2672.5944(7)
C / MHz 1959.52286(91) 1959.52222(12) 1959.5221(12)
ΔJ / kHz 3.2566(16) 3.25637(37) 3.258(7)
ΔJK / kHz −21.6019(19) −21.59241(82) −21.51(23)
ΔK / kHz 46.324(22) 46.1525(56) 45.7(4)
δJ / kHz 1.18701(14) 1.187996(38) 1.190(3)
δK / kHz 3.7917(28) 3.7715(13) 3.7(5)
ΦJ / Hz 0.0176(10) 0.01710(33)
ΦJK / Hz −0.0532(39) −0.0271(25)
ΦKJ / Hz −0.487(14) −0.4821(77)
ΦK / Hz 2.98(16) 1.951(44)
ϕJ / Hz 0.007386(90) 0.008079(46)
ϕJK / Hz 0.0346(33) 0.0117(20)
ϕK / Hz 0.404(28) 0.602(18)
LJK / mHz 0.088(10) 0.0462(17)
LK / mHz −4.62(48) −2.65(14)
lJK / mHz 0.0312(55)

χaa / MHz 0.0598(19) 0.0579(15)
(χbb − χcc) / MHz −4.6868(30) −4.688(2)
σfit / kHz 41.1 27.5 2.8
Nlines 537 4793 152
Jmin/Jmax 6/69 0/69 0/5
Ka, min/Ka, max 0/16 0/16 0/3

a Ground state analysis without taking the hyperfine structure into consideration. In the case of observable splitting, the central frequency is used. b Ground state analysis taking all hyperfine components into consideration, including those overlapped and the data from Halter et al. (2001) up to 14 GHz.

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