Abstract
A thermodynamic theory is presented to model the phase transitions and properties of lead zirconate. The free energy ΔG is expressed as a power series in terms of the ferroelectric polarization (Pi=P ai+Pbi) and antiferroelectric polarization (p i=Pai-Pbi) including all possible terms up to the sixth power, but only first-order cross coupling terms and couplings to elastic stress. Under the assumption that only the lowest-order coefficients of Pi and pi are linearly temperature dependent (Curie-Weiss behavior) and all other constants are temperature independent, experimental data are used to define the constants and permit calculation of ferroelectric and antiferroelectric free energies as a function of temperature. Use of the function to define the averaged dielectric permittivity at room temperature in the antiferroelectric phase gives a value of εR=120 in good agreement with recent microwave measurements. A simplified technique for modifying the function to explore solid solution with lead titanate is examined, and shown to lead to excellent agreement with the known phase diagram.
Original language | English (US) |
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Pages (from-to) | 3173-3180 |
Number of pages | 8 |
Journal | Journal of Applied Physics |
Volume | 65 |
Issue number | 8 |
DOIs | |
State | Published - 1989 |
All Science Journal Classification (ASJC) codes
- General Physics and Astronomy