Keywords :
Anharmonicities; Antiferrodistortive; Atomic motion; Brillouin zone boundary; Cubic structure; Quantum fluctuation; Soft modes; Soft-phonon mode; Temperature dependence; Theoretical study; Electronic, Optical and Magnetic Materials; Condensed Matter Physics; Physics - Materials Science
Abstract :
[en] Barium zirconate (BaZrO3) is one of the very few perovskites that is claimed to retain an average cubic structure down to 0K, while being energetically very close to an antiferrodistortive phase obtained by condensation of a soft phonon mode at the R point of the Brillouin zone boundary. In this work, we report a combined experimental and theoretical study of the temperature dependence of this soft phonon mode. Inelastic neutron and x-ray scattering measurements on single crystals show that it softens substantially from 9.4meV at room temperature to 5.6meV at 2K. In contrast, the acoustic mode at the same R point is nearly temperature independent. The effect of the anharmonicity on the lattice dynamics is investigated nonperturbatively using direct dynamic simulations as well as a first-principles-based self-consistent phonon theory, including quantum fluctuations of the atomic motion. By adding cubic and quartic anharmonic force constants, quantitative agreement with the neutron data for the temperature dependence of the antiferrodistortive mode is obtained. The quantum fluctuations of the atomic motion are found to be important to obtain the proper temperature dependence at low temperatures. The mean-squared displacements of the different atoms are determined as function of temperature and are shown to be consistent with available experimental data. Adding anharmonicity to the computed fluctuations of the Ba-O distances also improves the comparison with available extended x-ray absorption fine structure data at 300K.
Funding text :
R. Haumont and R. Saint-Martin from the ICMMO-UMR 8182, Université Paris Saclay, are acknowledged for their help in the preparation of the single crystals used for the INS experiments. F. Eriksson and P. Erhart are thanked for useful discussions in connection to the software hiphive . Funding from the Swedish Energy Agency (Grant No. 45410-1), the Swedish Research Council (Grants No. 2018-06482 and No. 2020-04935), and the Excellence Initiative Nano at Chalmers is gratefully acknowledged. The computations were performed by resources provided by the Swedish National Infrastructure for Computing (SNIC), partially funded by the Swedish Research Council through Grant Agreement No. 2018-05973. C. Milesi-Brault was supported by the Operational Programme Research, Development, and Education (financed by European Structural and Investment Funds and by the Czech Ministry of Education, Youth, and Sports), Project No. SOLID21-CZ.02.1.01/0.0/0.0/16_019/0000760.
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