Abstract
Complex permittivity ε* has been studied in the vicinity of the SmA-SmC* phase transition for samples 6, 12, 25, 50, and 100 μm thick. In the studied frequency range of (101−106) Hz the relaxation of collective modes, namely the soft, Goldstone and/or “thickness” modes, occurs. From the frequency dependence of ε* the relaxation frequency, fr , and dielectric strength, Δε, of these modes are determined in dependence of temperature and the sample thickness. Results are discussed on the basis of a phenomenological theory taking into account surface interactions.