Landau thermodynamic potential for BaTiO_3

TL;DR

This paper develops an eighth-power Landau thermodynamic potential for BaTiO_3 that accurately models its dielectric and ferroelectric properties across different phases, emphasizing the importance of higher-order and temperature-dependent coefficients.

Contribution

The study introduces an eighth-power Landau potential with temperature-dependent coefficients, improving the modeling of BaTiO_3's dielectric and ferroelectric behavior over previous lower-order potentials.

Findings

Eighth-power expansion better reproduces experimental data.

Temperature dependence of anharmonic coefficients is significant.

Proposed potential outperforms existing models in accuracy.

Abstract

In the paper, the description of the dielectric and ferroelectric properties of BaTiO_3 single crystals using Landau thermodynamic potential is addressed. Our results suggest that when using the sixth-power free energy expansion of the thermodynamic potential, remarkably different values of the fourth-power coefficient, \beta (the coefficient of P^4_i terms), are required to adequately reproduce the nonlinear dielectric behavior of the paraelectric phase and the electric field induced ferroelectric phase, respectively. In contrast, the eighth-power expansion with a common set of coefficients enables a good description for both phases at the same time. These features, together with the data available in literature, strongly attest to the necessity of the eighth-power terms in Landau thermodynamic potential of BaTiO_3. In addition, the fourth-power coefficients, \beta and \xi (the coefficient of P^2_i P^2_j terms), were evaluated from the nonlinear dielectric responses along [001], [011], and [111] orientations in the paraelectric phase. Appreciable temperature dependence was evidenced for both coefficients above T_C. Further analysis on the linear dielectric response of the single domain crystal in the tetragonal phase demonstrated that temperature dependent anharmonic coefficients are also necessary for an adequate description of the dielectric behavior in the ferroelectric phase. As a consequence, an eighth-power thermodynamic potential, with some of the anharmonic coefficients being temperature dependent, was proposed and compared with the existing potentials. In general, the potential proposed in this work exhibits a higher quality in reproducing the dielectric and ferroelectric properties of this prototypic ferroelectric substance.