The rotational spectra of ((OCS)-O-18)(3) and ((OCS)-C-13)(3) have been ass
igned using a pulsed-nozzle Fourier transform microwave spectrometer. The d
ata for these isotopic species have been combined with normal species data
from a paper by Connelly et al. [Connelly, J. P., et al. Mol Phys. 1996, 88
, 915] to determine the nine structural parameters of the trimer. The carbo
n atoms form a triangle with the axes of the monomer units roughly parallel
to each other (barrel-like structure). The monomers have an antiparallel-l
ike arrangement, with the dipole moment of one monomer opposing those of th
e ether two monomers. The dipole moment of the complex has been measured, g
iving values of mu(a) = 0.537(10) D, mu(c) = 0.373(2) D, and mu(total) = 0.
653(8) D. The b component of the dipole moment was too small to determine f
rom our data but is predicted to be about 0.02 D. The structure of (OCS)(3)
has been compared with similar trimers involving linear triatomic molecule
s and with the OCS dimer. Semiempirical calculations have been performed on
the (OCS)(3) system, and they show good qualitative agreement with the exp
erimental structure.