4.1 Article

Phonon spectra and phase transitions in van der Waals ferroics MM'P2X6

期刊

MOLECULAR CRYSTALS AND LIQUID CRYSTALS
卷 747, 期 1, 页码 14-22

出版社

TAYLOR & FRANCIS LTD
DOI: 10.1080/15421406.2022.2066787

关键词

Acoustic phonons; Brillouin scattering; CuInP2S6; flexoelectric coupling; frustrations; thermal conductivity; van der Waals ferroics

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The temperature dependence of longitudinal hypersound velocity in CuInP2S6 ferrielectrics was investigated using Brillouin spectroscopy. It was found that the acoustic phonon branch exhibits pronounced softening in the paraelectric phase below T* (approximately 330K) and cooling to the first order phase transition temperature T-c (approximately 312K) into the ferrielectric phase. The softening is induced by the flexoelectric coupling of relaxational soft polar optical and acoustic branches, which is related to an inhomogeneously polarized state appearing between the paraelectric and ferrielectric phases. The anomalous thermal conductivity of the CuInP2S6 crystal near the ferrielectric transition also demonstrates a decrease in the group velocity of heat transferring phonons with cooling from T* to T-c.
For CuInP2S6 ferrielectrics by Brillouin spectroscopy, the temperature dependence of the longitudinal hypersound velocity was investigated for the acoustic phonons propagated in plane of the crystal layers. Pronounced softening of acoustic phonon branch is observed in the paraelectric phase below T* approximate to 330 K at cooling to temperature T-c approximate to 312 K of the first order phase transition into ferrielectric phase. Below T-c the hypersound velocity growth in correlation with spontaneous polarization rise and its temperature anomaly is similar to earlier observed temperature behavior of longitudinal ultrasound velocity for acoustic wave propagated normally to the structural layers. Determined anomalous part of the CuInP2S6 crystal thermal conductivity in the vicinity of the ferrielectric transition also demonstrates lowering of the heat transferring phonons group velocity with cooling from T* to T-c. Observed acoustic softening obviously is induced by flexoelectric coupling of relaxational soft polar optical and acoustic branches that is related to an in ingomogeneously polarized state appearing between the paraelectric and ferrielectric phases.

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