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Table A.1

Molecular parameters for the Z and E isomer obtained from the XIAM analysis performed on the isolated non-overlapped rotational transitions.

Parameters Z isomer E isomer
A / MHz 9812.1817(25)a 9781.901(11)
B / MHz 4168.29145(24) 4189.37174(75)
C / MHz 2975.10391(31) 2983.1566(15)
ΔJ / kHz 0.77314(29) 0.76878(52)
ΔJK / kHz 15.6681(15) 15.0022(37)
ΔK / kHz -5.873(28) -5.920(56)
δJ / kHz 0.25747(13) 0.25119(22)
δK / kHz 9.4476(51) 8.979(11)
ΦJ / mHz [0.356]b [0.324]
ΦJK / Hz 0.1507(47) 0.17281(90)
ΦKJ / Hz -0.333(16) -0.4010(39)
ΦK / Hz [0.191]b [0.132]b
ϕJ / mHz [0.180]b [0.158]b
ϕJK / Hz 0.0694(13) 0.0566(22)
ϕK / Hz 0.364(33) [0.269]b
Dpi2− / MHz 0.203(21) 0.465(34)
V3 / cm−1 572.59(14) 508.05(22)
F0 / MHz [159.430]b [159.930]b
Iαc/uÅ2 [3.17]b [3.16]b
∠(i, a)c / ° 57.818(50) 61.682(97)
∠(i, b)c / ° 32.182(50) 28.318(97)
∠(i, c)c / ° [90.00]d [90.00]d
Jmin/Jmax 2 / 46 24 / 46
1 /16 0 / 25
A N/E Ne 192 /303 110 /149
σfitf / MHz 0.036 0.052
σwg / Unitless 1.054 1.594

Notes – (a)The numbers in parentheses are 1σ uncertainties in units of the last decimal digits. (b)Fixed to the calculated value, which is usually a preferred constraint against the zero or poorly determined value (Urban & Sarka 1990). (c)Derived parameter. (d)Fixed value due to Cs symmetry. (e)Number of A- and E-symmetry components in the fit.(f) Root mean square deviation of the fit. (g)Weighted deviation of the fit.

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