Abstract
First-principles calculations of various phases of CdTiO${}_{3}$ carried out with the aim of obtaining insights into the mechanism of the ferroelectric phase transition and the structure of the low-temperature ferroelectric phase are reported. The results indicate that the preferred symmetry of the low-temperature phase is Pna2${}_{1}$, rather than $P$2${}_{1}ma$, corresponding to a small relative shift of the Ti and O ions in the paraelectric Pnma phase with the polarization axis parallel to the long axis. Calculated phonon dispersion curves show a distinct soft mode at the \ensuremath{\Gamma} point of the Pnma phase, which vanishes in the Pna2${}_{1}$ phase, confirming that the transition to the ferroelectric phase is of the soft-mode displacive type. Calculations of perovskite CaTiO${}_{3}$, which also has an orthorhombic Pnma structure at room temperature but, unlike CdTiO${}_{3}$, does not exhibit a ferroelectric phase transition down to 4.2 K, were also carried out to help characterize the factors controlling ferroelectric phase transitions in perovskite titanates.
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