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. 2021 Mar 5;4:32. doi: 10.1038/s42004-021-00468-4

Table 2.

Observed spectroscopic parameters for homochiral and heterochiral dimers of styrene oxide.

[0]RRa [1]RRb [2]RS [3]RR [4]RS [7]RR
A/MHz 378.28285(20) 572.181(12) 476.41175(21) 519.837962(47) 565.132480(93) 512.20992(15)
B/MHz 330.824777(86) 386.3259(45) 399.70525(14) 350.271983(38) 327.768274(72) 360.88847(11)
C/MHz 249.305701(65) 276.86249(37) 371.57747(16) 322.618306(39) 307.883752(74) 302.976455(82)
DK/kHz −0.3622(31) −0.1967(63) −0.16430(21) 0.1576(11) −0.0235(37)
DJK/kHz 0.4531(14) 0.1363(66) 0.15629(25) −0.0458(13) −0.0180(28)
DJ/kHz 0.01625(30) 0.03487(93) 0.0758(14) 0.07994(16) 0.07401(34) 0.06366(55)
δK/kHz 0.23156(74) 0.3045(86) 0.0455(96) 0.1565(36)
δJ/kHz −0.00562(16) 0.00558(78) 0.00293(19) 0.00636(27)
μa y y n y y y
μb n y y y y y
μc n n y y y y
N 148 b 159 470 342 148
σ/kHz 3.7 6.8 5.6 4.7 4.9 3.1

Primary rotational constants (A,B,C) are given in MHz, and quartic centrifugal distortion constants are given in kHz. The errors for the measured values are standard errors. N is the number of lines included in the fit, and σ is the standard deviation of the fit. The experimental frequency accuracy is 25 kHz.

aRotational constants and centrifugal distortion constants for the global minimum geometry of the homochiral dimer of 2-(4-fluorophenyl)oxirane, which is predicted to be structurally equivalent to [0]RR (Supplementary Fig. 3).

bThe rotational constants shown for the [1]RR dimer correspond to a partial fit to the centre frequencies of a splitting pattern tentatively assigned to a large-amplitude motion inverting the a- and b-type dipole moment components.