A free energy landscape perspective on the nature of collective diffusion in amorphous solids

被引:35
|
作者
Wang, Yun-Jiang [1 ,2 ]
Du, Jun-Ping [3 ,4 ]
Shinzato, Shuhei [3 ]
Dai, Lan-Hong [1 ,2 ]
Ogata, Shigenobu [3 ,4 ]
机构
[1] Chinese Acad Sci, Inst Mech, State Key Lab Nonlinear Mech, Beijing 100190, Peoples R China
[2] Univ Chinese Acad Sci, Sch Engn Sci, Beijing 100049, Peoples R China
[3] Osaka Univ, Grad Sch Engn Sci, Dept Mech Sci & Bioengn, Osaka 5608531, Japan
[4] Kyoto Univ, Ctr Elements Strategy Initiat Struct Mat ESISM, Sakyo Ku, Kyoto 6068501, Japan
关键词
Metallic glasses; Collective diffusion; Accelerated molecular dynamics; Free energy landscape; METALLIC GLASSES; MOLECULAR-DYNAMICS; SUPERCOOLED LIQUIDS; COOPERATIVE MOTION; COPPER-ZIRCONIUM; SELF-DIFFUSION; STRAIN-RATE; ALLOYS; TRANSITION; MECHANISMS;
D O I
10.1016/j.actamat.2018.07.029
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
The nature of collective diffusion in amorphous solids is in strong contrast with diffusion in crystals. However, the atomic-scale mechanism and kinetics of such collective diffusion remains elusive. Here the free energy landscape of collective diffusion triggered by single atom hopping in a prototypical Cu50Zr50 metallic glass is explored with well-tempered metadynamics which significantly expands the observation timescale of diffusion at atomic-scale. We clarify an experimentally suggested collective atomic diffusion mechanism in the deep glassy state. The collective nature is strongly temperature-dependent. It evolves from string-like motion with only several atoms to be large size collective diffusion at high temperature, which can promote the atomic transport upon glass transition temperature. We also clarify the apparent diffusivity is dominated by the highest free energy barrier of atomic diffusion among widely distributed free energy barriers due to the dynamic heterogeneity of metallic glass, which suggests the sequential nature of diffusion is a proper assumption to the metallic glasses with dynamic heterogeneity. The temperature and pressure dependence of diffusion free energy landscape are further quantified with activation entropy, (19.6 +/- 2.5)k(B), and activation volume, (7.9 +/- 3.4) angstrom(3), which agree quantitatively with experiments. Laboratory timescale simulations of atomic diffusion brings physical insights into the unique atomic motion mechanism in non-crystalline materials. (C) 2018 Acta Materialia Inc. Published by Elsevier Ltd. All rights reserved.
引用
收藏
页码:165 / 173
页数:9
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