The pure rotational spectra of 4-methylthiazole···H
2
O and 5-methylthiazole···H
2
O were
recorded by chirped-pulse Fourier transform microwave (CP-FTMW) spectroscopy.
Each complex was generated within the rotationally cold environment
of a gas sample undergoing supersonic expansion in the presence of
an argon buffer gas. The spectra of five isotopologues of each complex
have been measured and analyzed to determine the rotational constants,
A
0
,
B
0
, and
C
0
; centrifugal distortion constants,
D
J
,
D
JK
, and
d
1
; nuclear quadrupole
coupling constants,
χ
aa
(N3) and [
χ
bb
(N3) –
χ
cc
(N3)]; and parameters describing the internal rotation of the CH
3
group,
V
3
and
∠
(
i
,
b
). The experimentally deduced
parameters were obtained using the XIAM and the BELGI-C
s
-hyperfine code. For each complex, parameters in the molecular geometry
are fitted to experimentally determined moments of inertia. DFT calculations
have been performed at the ωB97X-D/aug-cc-pVQZ level in support
of the experiments. Each complex contains two hydrogen bonds; a comparatively
strong, primary interaction between the N of thiazole and an O–H
of H
2
O, and a weaker, secondary interaction between O and
either the hydrogen atom attached to C2 (in 5-methylthiazole···H
2
O) or the CH
3
group attached to C4 (in 4-methylthiazole···H
2
O). The barrier to internal rotation of the CH
3
group,
V
3
, is slightly lower for 4-methylthiazole···H
2
O (XIAM result is 340.05(56) cm
–1
) than
that for the 4-methylthiazole monomer (357.6 cm
–1
). This is likely to be a result of internal charge redistribution
within the 4-methylthiazole subunit following its coordination by
H
2
O. At the precision of the experiments,
V
3
of 5-methylthiazole···H
2
O
(XIAM result is 325.16(38) cm
–1
) is not significantly
different from
V
3
of the 5-methylthiazole
monomer (332.0 cm
–1
).