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. Author manuscript; available in PMC: 2019 May 9.
Published in final edited form as: J Mol Spectrosc. 2017;342:10.1016/j.jms.2017.06.008. doi: 10.1016/j.jms.2017.06.008

Table 2.

Fourier expansion coefficientsa for ab initio calculated elements of the symmetry-adapted spin-rotation hyperfine tensor in kHz for the methyl and hydroxyl hydrogensb in CH3CHO.

Ea,Ebc C1 C2 C4 × 101 C5 × 101 C7 × 102 C8 × 102 σ × 1033
H654aa −2.668541(60) 0.864234(60) −1.08354(60) 0.44347(60) −0.8347(60) 0.3299(60) 0.5
H654bb 0.4481511(98) 0.5711596(98) −0.211404(95) 0.091996(95) −0.16789(96) 0.04523(96) 0.1
H654cc 0.0056904(59) −0.6150126(73) 0.269017(63) −0.131423(93) 0.18017(90) −0.07179(64) 0.07
H654ab 1.046126(26) −0.902223(28) 0.55623(26) −0.34093(27) 0.4585(27) −0.2548(26) 0.2
Ea,Ebd C1 C2 C4 × 101 C5 × 101 C7 × 102 C8 × 102 σ × 103
H654bc −0.1988570(78) −0.5978437(72) 0.233788(74) −0.111522(74) 0.16445(72) −0.05854(76) 0.07
H654ac −1.546908(19) 1.006859(19) −0.69420(22) 0.39498(22) −0.5217(19) 0.2713(19) 0.08
A1e C0 C3 × 101 C6 × 102 C9 × 103 σ × 103
H654aa −4.4080943(43) −0.306366(60) −0.39178(60) −0.5152(60) 0.05
H654bb −0.60920230(46) 0.0565405(56) 0.050860(70) 0.05137(60) 0.005
H654cc −0.51296483(53) 0.0041913(92) 0.007482(58) 0.03878(85) 0.005
H654ab −0.33233713(57) −0.4509870(64) −0.064574(66) −0.01392(77) 0.004
H1aa −4.4691361(37) −1.006584(51) −0.46249(51) −0.4415(51) 0.04
H1bb 1.12733677(77) −0.080874(11) −0.07824(11) −0.0750(11) 0.009
H1cc −0.71453571(55) −0.1215039(76) −0.018540(76) 0.02373(76) 0.007
H1ab 0.3546764(23) −0.519036(32) −0.22522(32) −0.1980(32) 0.03
A2f C3 × 101
H654bc −0.02669(24) 0.2
H654ac 0.30515(47) 0.3
H1bc Small
H1ac Small
a

The last two letters in symbols like H654aa, H1aa, etc. indicate tensor components labeled by the a,b,c principal axes of the molecule. Off-diagonal tensor elements labeled ab, bc, or ac are actually the averages (1/2)(ab+ba), etc. Numbers in parentheses are one standard uncertainty in the last two digits (type A, k = 1) [13]; σ is the overall standard deviation of the fit in kHz. Some expansion coefficients cannot be well determined because the corresponding spin-rotation hyperfine tensor components fall below a printout cut-off in Gaussian for some values of the internal rotation angle.

b

H654 and H1 indicate spin-rotation constants for the three methyl H atoms and for the hydroxyl H atom, respectively.

c

Spin-rotation tensor elements of species E. The Ea and Eb components are expanded as C1 cosσ + C2 cos2σ + C4 cos4σ + C5 cos5σ and – C1 sinα + C2 sin2α – C4 sin4α + C5 sin5α, respectively.

d

Spin-rotation tensor elements of species E. Ea and Eb components are expanded as C1 sinα + C2 sin2α + C4 sin4α + C5 sin5α and C1 cosα – C2 cos2α + C4 cos4α – C5 cos5α, respectively.

e

Spin-rotation tensor elements of species A1, with Fourier expansions in C3n cos3nα.

f

Spin-rotation tensor elements of species A2, with Fourier expansions in C3n sin3nα.