Shang B S, Li M Z, Yao Y G, Lu Y J, Wang W H
State Key Laboratory of Nonlinear Mechanics, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100190, China.
Department of Physics, Renmin University of China, Beijing 100872, China.
Phys Rev E Stat Nonlin Soft Matter Phys. 2014 Oct;90(4):042303. doi: 10.1103/PhysRevE.90.042303. Epub 2014 Oct 7.
Atomic rearrangements induced by shear stress are fundamental for understanding deformation mechanisms in metallic glasses (MGs). Using molecular dynamic simulation, the atomic rearrangements characterized by nonaffine displacements (NADs) and their spatial distribution and evolution with tensile stress in Cu50Zr50 MG were investigated. It was found that in the elastic regime the atomic rearrangements with the largest NADs are relatively homogeneous in space, but exhibit strong spatial correlation, become localized and inhomogeneous, and form large clusters as strain increases, which may facilitate the so-called shear transformation zones. Furthermore, initially they prefer to take place around Cu atoms which have more nonicosahedral configurations. As strain increases, the preference decays and disappears in the plastic regime. The atomic rearrangements with the smallest NADs are preferentially located around Cu atoms, too, but with more icosahedral or icosahedral-like atomic configurations. The preference is maintained in the whole deformation process. In contrast, the atomic rearrangements with moderate NADs distribute homogeneously, and do not show explicit preference or spatial correlation, acting as matrix during deformation. Among the atomic rearrangements with different NADs, those with largest and smallest NADs are nearest neighbors initially, but separating with increasing strain, while those with largest and moderate NADs always avoid to each other. The correlations in the fluctuations of the NADs confirm the long-range strain correlation and the scale-free characteristic of NADs in both elastic and plastic deformation, which suggests a universality of the scaling in the plastic flow in MGs.
由剪切应力引起的原子重排是理解金属玻璃(MGs)变形机制的基础。利用分子动力学模拟,研究了以非仿射位移(NADs)为特征的原子重排及其在Cu50Zr50金属玻璃中随拉伸应力的空间分布和演化。研究发现,在弹性阶段,具有最大NADs的原子重排在空间上相对均匀,但表现出很强的空间相关性,随着应变增加变得局部化且不均匀,并形成大的团簇,这可能促进所谓的剪切转变区。此外,最初它们倾向于在具有更多非二十面体构型的Cu原子周围发生。随着应变增加,这种偏好逐渐减弱并在塑性阶段消失。具有最小NADs的原子重排也优先位于Cu原子周围,但具有更多二十面体或类二十面体的原子构型。这种偏好在整个变形过程中保持。相比之下,具有中等NADs的原子重排均匀分布,没有表现出明显的偏好或空间相关性,在变形过程中起基体作用。在具有不同NADs的原子重排中,具有最大和最小NADs的那些最初是最近邻,但随着应变增加而分离,而具有最大和中等NADs的那些总是相互避开。NADs波动中的相关性证实了弹性和塑性变形中NADs的长程应变相关性和无标度特性,这表明金属玻璃塑性流动中尺度缩放的普遍性。