Abstract
Evidence of a first-order smectic-A–smectic- (SmA-Sm) transition is presented. Detailed x-ray studies on 4-(3-methyl-2-chloropentanoyloxy)4’-heptyloxybiphenyl show that the SmA-Sm transition in this material is characterized by a discontinuous jump in the layer spacing (and hence in the tilt angle) and by a narrow two-phase region in which the density modulations due to the smectic-A and the smectic- phases coexist. Addition of a second compound drives the SmA-Sm transition towards second order.
- Received 30 November 1987
DOI:https://doi.org/10.1103/PhysRevA.37.1824
©1988 American Physical Society