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    Finite-temperature lattice dynamics of PbZrO3

    Kinnary Patel1, Bin Xu2, Sergey Prosandeev1, and Laurent Bellaiche1,3

    • 1Smart Ferroic Materials Center, Department of Physics and Arkansas Materials Institute, University of Arkansas, Fayetteville, Arkansas 72701, USA
    • 2Jiangsu Key Laboratory of Frontier Material Physics and Devices, Jiangsu Key Laboratory of Advanced Negative Carbon Technologies, School of Physical Science and Technology, Soochow University, Suzhou 215006, China
    • 3Department of Materials Science and Engineering, Tel Aviv University, Ramat Aviv, Tel Aviv 6997801, Israel

    Phys. Rev. B 114, 274101 – Published 2 November, 2026

    DOI: https://doi.org/10.1103/lysd-79xd

    Abstract

    We investigate the temperature-dependent dynamical properties of PbZrO3 (PZO) using molecular dynamics (MD) simulations with an effective Hamiltonian. As temperature decreases from 1800  to 10 K, PZO is predicted to undergo a sequence of phase transitions. Above 1350 K, it exhibits the cubic paraelectric Pm3¯m phase. Between 1350  and 650 K, an intermediate phase emerges, denoted here as the Σ phase and characterized by antipolar displacements along [110] and complex oxygen octahedral tiltings about [001], both associated with the Σ point and with amplitudes increasing upon cooling. Below 650 K, PZO stabilizes in the Pbam ground state, exhibiting additional R- and S4-point order parameters, with all associated condensed degrees of freedom strengthening at lower temperatures. MD results yield a first-order character of the Pm3¯m-to-Σ and Σ-to-Pbam transitions. Moreover, phonon analysis reveals the predicted temperature evolution of mode frequencies associated with Γ, R, Σ, and S4k points. In the cubic phase, Σ, mode having both antipolar and octahedral tiltings characteristics is softening on temperature decrease, as consistent with the existence of a bilinear coupling that is often overlooked. In the Σ phase, a mode associated with the R-point-induced antiphase octahedral tiltings strongly softens. Within the Pbam phase, multiple resonant frequencies appear for each mode, reflecting complex mode couplings, including bilinear and trilinear ones. These computations agree well with experimental data, including temperature behavior of soft mode and even a higher mode, which calls for testing all present predictions, that may offer new insight into key features of PZOs including its lattice dynamics and phase transitions.

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