We have performed a structural study of the liquid crystal (LC) octylc
yanobiphenyl (8CB), deposited on gratings and flat surfaces, using hig
h resolution X-ray scattering as a function of film thickness. 8CB is
a room temperature smectic A2', with a layer spacing of 31.6 angstrom.
Glass was used as substrate and treated with either one of the organi
c surfactants MAP or DMOAP. Surface tension forces cause the liquid cr
ystal molecules to align perpendicularly with respect to the plane of
the substrate at the air interface. Competing with the LC-air interfac
e, which is a strong aligner, a grating at the LC-substrate interface
produces distortions in the smectic layering with an excess of elastic
energy, which favours alignment parallel to the substrate and the gro
oves. Our purpose was to detect the onset and evolution of parallel al
ignment as a function of film thickness. The studies used 9 keV (1.403
angstrom) X-rays focused to a spot size of 2 mm2 at the sample positi
on. In-plane scans, which detect the smectic layers perpendicular to t
he plane of the substrate, were done at angles phi = 0-degrees and 90-
degrees with respect to the gratings to ascertain the molecular orient
ation, at a nominal X-ray incidence angle of alpha = 0-degrees. In ord
er to observe regions of varying smectic layer orientation within the
film, we performed a series of scans where the out-of-plane tilt angle
chi changed from 0-degrees, corresponding to scattering in the plane
of the film, to 90-degrees, which corresponds to scattering normal to
the surface of the film. The results from these scans were fitted to a
multilayer model where the orientation of the smectic layers varies a
s a function of film depth. The analysis confirmed our earlier observa
tions that surface tension at the air interface plays a dominant role
in the alignment of the LC molecules.