Fig. 2.

Left: section of the rotational spectrum of EMS showing the 190, 19–181, 18 and 162, 15–152, 14 rotational transitions for trans and gauche conformers, respectively. For these transitions, the A − E splittings are irresolvable since they are smaller than the experimental broadening of the lines. The negative features marked with an asterisk are produced by the folding of the frequency-switched data and appear at ±25 MHz of each rotational transition. Middle: 363, 33–362, 34b-type Q-branch rotational transition for the trans conformer of EMS where the A − E splittings can be observed. Right: 335, 28–334, 29b-type Q-branch rotational transition for the gauche conformer of EMS with the A − E internal rotation components indicated.
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