The structural interaction in a presmectic film is analyzed theoretically u
sing the Cartesian rather than the polar representation of the smectic orde
r parameter. This representation diagonalizes the phenomenological Hamilton
ian of the ordering and leads to a unified description of the mean-held int
eraction-first studied by de Gennes [Langmuir 6, 1448 (1990)]-and the fluct
uation-induced interaction, The fluctuation-induced interaction turns out t
o be short-range, attractive, and unaffected by the apparent bidomain struc
ture of the film, which controls the oscillatory mean-held interaction.