Abstract
Ferroelectric materials are characterized by a finite electric polarization in absence of an external electric field. Furthermore, this polarization must possess at least two stable states, and must have the ability to be reversibly switched from one state to another by the application of an electric field.
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Notes
- 1.
Some ferroelectric materials rather undergo a ferroelectric phase transition from a microscopically polar but macroscopically nonpolar high temperature phase (so-called order-disorder phase transition), and in some cases the phase transition can exhibit both characters together.
- 2.
The cubic group 432, although noncentrosymmetric, has other symmetry elements that exclude piezoelectricity.
- 3.
The order parameter may be a scalar, a vector, a complex number, or a more complicated quantity. For the purpose of simplicity, we will take it to be a scalar in the present demonstration.
- 4.
Landau’s theory considers the Helmoltz free energy \(F\); instead, one can also expand the Gibbs free energy \(G(p,T,\psi )\) to get pressure- and temperature-dependent coefficients.
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Guyonnet, J. (2014). Domain Walls in Ferroelectric Materials. In: Ferroelectric Domain Walls. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-319-05750-7_2
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