Switching of banana liquid crystal mesophases under field

• Published in: The European physical journal. E, Soft matter and biological physics Soft matter and biological physics, 2003-02, Vol.10 (2), p.129-134
• Main Authors: ACHARD, M. F, BEDEL, J. Ph, MARCEROU, J. P, NGUYEN, H. T, ROUILLON, J. C
• Format: Article
• Language: English
• Subjects: Condensed matter: electronic structure, electrical, magnetic, and optical properties; Condensed matter: structure, mechanical and thermal properties; Dielectric, piezoelectric, ferroelectric and antiferroelectric materials; Dielectrics, piezoelectrics, and ferroelectrics and their properties; Exact sciences and technology; Liquid crystals; Liquids and liquid crystals; Liquids, emulsions, and suspensions; liquid crystals; Orientational order of liquid crystals; electric and magnetic field effects on order; Physics; Structure of solids and liquids; crystallography
• ISSN: 1292-8941; 1292-895X
• DOI: 10.1140/epje/e2003-00016-y

Taking advantage of the great number of bent-core or "banana" compounds synthesized and studied in the laboratory, we describe their behaviour under the application of an external electric field. If the field were a static one, we would work within the frame of an equilibrium phase diagram in a (field E, temperature T) space where some phases would be simple dielectrics and others ferroelectric ones with a macroscopic polarization, either spontaneous or induced by the field. In this paper, we deal with the basic responses of "banana" liquid crystals under the application of a low frequency (1 to 100 Hz) AC field. Firstly square-wave voltages allow us to locate the phase boundary between dielectric (at lower field) and ferroelectric phases (higher field) at a given temperature and field threshold. Then we apply slowly varying AC voltages with shapes like triangle or "triple-plateau" to check out the stability of the induced ferroelectric phase versus field removal. Three behaviours are encountered, the unstable one (short lifetime of the high-field ferroelectric phase) where the macroscopic polarization is destroyed and then rebuilt in the opposite direction during each half period and usually called "antiferroelectric"; the stable one (long lifetime) with a polarization that rotates at constant modulus which is labeled as "ferroelectric" and a new one where the macroscopic polarization is proportional to the applied field, we named this behaviour as "superparaelectric". Let us stress that these observations apply to the ferroelectric phases of the (E, T) phase diagram not to the zero field (0,T) phases observed in the usual phase characterization experiments except for an eventual spontaneous ferroelectric phase.