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晶型多态体中原子扩散机制与整体输运系数之间的关系。

Relationships between atomic diffusion mechanisms and ensemble transport coefficients in crystalline polymorphs.

机构信息

Department of Materials, University of Oxford, Parks Road, Oxford OX1 3PH, United Kingdom and Stephenson Institute for Renewable Energy, Department of Chemistry, University of Liverpool, Liverpool L69 3BX, United Kingdom.

Department of Materials, University of Oxford, Parks Road, Oxford OX1 3PH, United Kingdom.

出版信息

Phys Rev Lett. 2014 Apr 11;112(14):145901. doi: 10.1103/PhysRevLett.112.145901. Epub 2014 Apr 8.

Abstract

Ionic transport in conventional ionic solids is generally considered to proceed via independent diffusion events or "hops." This assumption leads to well-known Arrhenius expressions for transport coefficients, and is equivalent to assuming diffusion is a Poisson process. Using molecular dynamics simulations of the low-temperature B1, B3, and B4 AgI polymorphs, we have compared rates of ion hopping with corresponding Poisson distributions to test the assumption of independent hopping in these common structure types. In all cases diffusion is a non-Poisson process, and hopping is strongly correlated in time. In B1 the diffusion coefficient can be approximated by an Arrhenius expression, though the physical significance of the parameters differs from that commonly assumed. In low temperature B3 and B4, diffusion is characterized by concerted motion of multiple ions in short closed loops. Diffusion coefficients cannot be expressed in a simple Arrhenius form dependent on single-ion free energies, and intrinsic diffusion must be considered a many-body process.

摘要

在传统的离子固体中,离子输运通常被认为是通过独立的扩散事件或“跳跃”来进行的。这种假设导致了著名的 Arrhenius 输运系数表达式,并且等效于假设扩散是泊松过程。通过对低温 B1、B3 和 B4 碘化银多晶型体的分子动力学模拟,我们比较了离子跳跃的速率与相应的泊松分布,以检验这些常见结构类型中独立跳跃的假设。在所有情况下,扩散都不是泊松过程,跳跃在时间上具有很强的相关性。在 B1 中,扩散系数可以用 Arrhenius 表达式近似,尽管参数的物理意义与通常假设的不同。在低温 B3 和 B4 中,扩散的特征是多个离子在短闭合环中协同运动。扩散系数不能用简单的 Arrhenius 形式表示,依赖于单离子自由能,并且必须将本征扩散视为多体过程。

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