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颗粒状物理凝胶的声子输运特性

Phonon transport properties of particulate physical gels.

作者信息

Mizuno Hideyuki, Hachiya Makoto, Ikeda Atsushi

机构信息

Graduate School of Arts and Sciences, The University of Tokyo, Tokyo 153-8902, Japan.

出版信息

J Chem Phys. 2022 May 28;156(20):204505. doi: 10.1063/5.0090233.

Abstract

Particulate physical gels are sparse, low-density amorphous materials in which clusters of glasses are connected to form a heterogeneous network structure. This structure is characterized by two length scales, ξ and ξ: ξ measures the length of heterogeneities in the network structure and ξ is the size of glassy clusters. Accordingly, the vibrational states (eigenmodes) of such a material also exhibit a multiscale nature with two characteristic frequencies, ω and ω, which are associated with ξ and ξ, respectively: (i) phonon-like vibrations in the homogeneous medium at ω<ω, (ii) phonon-like vibrations in the heterogeneous medium at ω<ω<ω, and (iii) disordered vibrations in the glassy clusters at ω > ω. Here, we demonstrate that the multiscale characteristics seen in the static structures and vibrational states also extend to the phonon transport properties. Phonon transport exhibits two distinct crossovers at frequencies ω and ω (or at wavenumbers of ∼ξ and ∼ξ ). In particular, both transverse and longitudinal phonons cross over between Rayleigh scattering at ω<ω and diffusive damping at ω>ω. Remarkably, the Ioffe-Regel limit is located at the very low frequency of ω. Thus, phonon transport is localized above ω, even where phonon-like vibrational states persist. This markedly strong scattering behavior is caused by the sparse, porous structure of the gel.

摘要

颗粒状物理凝胶是稀疏的低密度非晶材料,其中玻璃态簇相互连接形成异质网络结构。这种结构具有两个长度尺度,ξ 和 ξ:ξ 衡量网络结构中不均匀性的长度,ξ 是玻璃态簇的尺寸。因此,这种材料的振动状态(本征模)也呈现出具有两个特征频率 ω 和 ω 的多尺度性质,它们分别与 ξ 和 ξ 相关:(i)在 ω<ω 时,均匀介质中的类声子振动;(ii)在 ω<ω<ω 时,异质介质中的类声子振动;(iii)在 ω > ω 时,玻璃态簇中的无序振动。在此,我们证明在静态结构和振动状态中看到的多尺度特征也延伸到了声子输运性质。声子输运在频率 ω 和 ω(或在波数 ∼ξ 和 ∼ξ 处)表现出两个明显的转变。特别是,横向和纵向声子在 ω<ω 时的瑞利散射和 ω>ω 时的扩散阻尼之间发生转变。值得注意的是,伊夫 - 雷格尔极限位于非常低的频率 ω 处。因此,即使类声子振动状态持续存在,声子输运在 ω 以上也是局域化的。这种明显强烈的散射行为是由凝胶的稀疏、多孔结构引起的。

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