AntiferroelectricityPublished on 24/2/2012 and last updated on Wednesday 27th of June 2018 at 06:10:11 PM
The entire macroscopic spontaneous polarization in antiferroelectric material is zero. The reason is that the closest dipoles will cancel each other. This property can emerge or vanish depending on various parameters. The parameters are external field, pressure, growth method, temperature etc. The antiferroelectric property is not piezoelectric. That is there is no change in mechanical character of the material by the application of external field. These materials usually have high dielectric constant. The dipole orientation of this material is similar to the chess board pattern which is shown below.
Antiferroelectric MaterialsThe examples of antiferroelectric materials are as follows
- PbZrO3 (Lead Zirconate)
- NH4H2PO4 (ADP: Ammonium dihydrogen Phosphate)
- NaNbO3(Sodium Niobate)
Antiferroelectricity and TemperatureThe antiferroelectric property will vanish above a particular temperature. This we can call as Antiferroelectric Curie point. The materials and their curie temperature are shown in Table no.1. The dielectric constant (relative permittivity) less and more than this Curie point is investigated. This is done for both first and second order transition. In the second order transition, dielectric constant is continuous all over the Curie point. In the two cases dielectric constant must not be very high.
Double Hysteresis LoopThe hysteresis loop of a perfect antiferroelectric material can be drawn as shown in Figure 2 below. The reversal of spontaneous polarization of these materials gives a double hysteresis loops. The external field applied is a low frequency AC field.
Application of Antiferroelectricity
- Super capacitors
- MEMS Application
- Used in integration with ferromagnetic materials
- High energy storage devices
- Photonic application
- Liquid crystal etc.