The rotational transition frequencies were mostly
taken from
(1) L. Kolesniková, J. L. Alonso, C. Bermúdez,
E. R. Alonso, B. Tercero, J. Cernicharo, and J.-C. Guillemin,
2016, Astron. Astrophys. 591, Art. No. A75.
Four hyperfine-free microwave transition frequencies were
taken from
(2) M. Y. Fong, L. J. Johnson, and M. D. Harmony,
1974, J. Mol. Spectrosc. 53, 45.
The parameter set differs slightly from that in (1).
The uncertainties from that work were slightly conservative
and were adjusted. The experimental lines were not merged,
but the can be inspected in the archive directory.
Please note that erham sometimes mislabels transitions.
Hyperfine structure splitting is not provided. It is likely
very small except for some transitions having very small
quantum numbers.
The molecules displays commonly splitting caused by methyl
internal rotation; state number 0 signals the A
symmetry component, 1 the E symmetry component.
Calculations with uncertainties exceeding 0.3 MHz should
be viewed with substantial caution.
The dipole moment components were derived from a
quantum-chemical calcultion by
(3) H. S. P. Müller, 2020, unpublished.
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