Rayleigh scattering and disorder-induced mixing of polarizations in amorphous solids at the nanoscale: 1-octyl-3-methylimidazolium chloride glass

M. G. Izzo, B. Wehinger, S. Cazzato, A. Matic, C. Masciovecchio, A. Gessini, G. Ruocco
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引用次数: 2

Abstract

Acoustic excitations in topologically disordered media at mesoscale present anomalous features with respect to the Debye's theory. In a three-dimensional medium an acoustic excitation is characterized by its phase velocity, intensity and polarization. The so-called Rayleigh anomalies, which manifest in attenuation and retardation of the acoustic excitations, affect the first two properties. The topological disorder is, however, expected to influence also the third one. Acoustic excitations with a well-defined polarization in the continuum limit present indeed a so-called mixing of polarizations at nanoscale, as attested by experimental observations and Molecular Dynamics simulations. We provide a comprehensive experimental characterization of acoustic dynamics properties of a selected glass, 1-octyl-3-methylimidazolium chloride glass, whose heterogeneous structure at nanoscale is well-assessed. Distinctive features, which can be related to the occurrence of the Rayleigh anomalies and of the mixing of polarizations are observed. We develop, in the framework of the Random Media Theory, an analytical model that allows a quantitative description of all the Rayleigh anomalies and the mixing of polarizations. Contrast between theoretical and experimental features for the selected glass reveals an excellent agreement. The quantitative theoretical approach permits thus to demonstrate how the mixing of polarizations generates distinctive feature in the dynamic structure factor of glasses and to unambiguously identify them. The robustness of the proposed theoretical approach is validated by its ability to describe as well transverse acoustic dynamics.
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纳米尺度下非晶固体中瑞利散射和无序极化混合:1-辛基-3-甲基咪唑氯玻璃
相对于德拜理论,中尺度拓扑无序介质中的声激励表现出异常特征。在三维介质中,声激励的特征是相速度、强度和极化。所谓的瑞利异常,表现为声激励的衰减和延迟,影响前两种性质。然而,预计拓扑紊乱也会影响第三种紊乱。实验观察和分子动力学模拟证明,在连续统极限下具有明确极化的声激励确实存在所谓的纳米级极化混合。我们对选定的1-辛基和3-甲基咪唑氯玻璃的声学动力学特性进行了全面的实验表征,并对其在纳米尺度上的非均相结构进行了很好的评估。观察到与瑞利异常的发生和极化混合有关的显著特征。在随机介质理论的框架内,我们开发了一个分析模型,该模型允许对所有瑞利异常和极化混合进行定量描述。所选玻璃的理论特征和实验特征的对比显示出极好的一致性。因此,定量理论方法允许证明偏振混合如何在玻璃的动态结构因子中产生独特的特征,并明确地识别它们。所提出的理论方法的鲁棒性通过其描述横向声动力学的能力得到验证。
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