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Spin-phonon coupling and high-temperature phase transition in multiferroic material YMnO3

机译:多铁性材料YMnO3中的自旋声子耦合和高温相变

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We have carried out temperature-dependent inelastic neutron scattering measurements of YMnO3 over the temperature range of 50-1303 K, covering both the antiferromagnetic to paramagnetic transition (70 K), as well as the ferroelectric to paraelectric transition (1258 K). Measurements are accompanied by first principles calculations of phonon spectra for the sake of interpretation and analysis of the measured phonon spectra in the room temperature ferroelectric (P6(3)cm) and high temperature paraelectric (P6(3)/mmc) hexagonal phases of YMnO3. The comparison of the experimental and first-principles calculated phonon spectra highlights unambiguously a spin-phonon coupling character in YMnO3. This is further supported by the pronounced differences in the magnetic and non-magnetic phonon calculations. The calculated atomistic partial phonon contributions of the Y and Mn atoms are not affected by the inclusion of magnetic interactions, whereas the dynamical contribution of the O atoms is found to change. This highlights the role of the super-exchange interactions between the magnetic Mn cations, mediated by O bridges. Phonon dispersion relations have also been calculated, in the entire Brillouin zone, for both the hexagonal phases. In the high-temperature phase, unstable phonon mode at the K point is highlighted. The displacement pattern at the K-point indicates that the freezing of this mode along with the stable mode at the G-point may lead to a stabilization of the low-temperature (P6(3)cm) phase, inducing ferroelectricity. Furthermore, we have also estimated the mode Gruneisen parameter and volume thermal expansion behavior. The latter is found to agree with the available experimental data.
机译:我们已经在50-1303 K的温度范围内对YMnO3进行了随温度变化的非弹性中子散射测量,涵盖了反铁磁到顺磁转变(70 K)以及铁电到顺电转变(1258 K)。测量过程中伴随着声子光谱的第一性原理计算,以便解释和分析YMnO3的室温铁电(P6(3)cm)和高温顺电(P6(3)/ mmc)六角相中的声子光谱。实验原理和第一性原理计算的声子光谱的比较清楚地突出了YMnO3中的自旋声子耦合特性。磁性和非磁性声子计算中的明显差异进一步证明了这一点。 Y和Mn原子的计算得出的原子性部分声子贡献不受磁相互作用的影响,而O原子的动力学贡献却发生了变化。这突显了由O桥介导的磁性Mn阳离子之间的超交换相互作用的作用。还已经在整个布里渊区中为两个六角相计算了声子色散关系。在高温阶段,突出显示K点的不稳定声子模式。在K点的位移模式表明,该模式的冻结以及在G点的稳定模式可能导致低温(P6(3)cm)相的稳定,从而引发铁电。此外,我们还估算了模式Gruneisen参数和体积热膨胀行为。发现后者与可用的实验数据一致。

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