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通过第一性原理局部能量和局部应力分析 Fe 晶粒边界的 Si 偏析。

Si segregation at Fe grain boundaries analyzed by ab initio local energy and local stress.

机构信息

Research Institute for Ubiquitous Energy Devices, National Institute of Advanced Industrial Science and Technology (AIST), 1-8-31 Midorigaoka, Ikeda, Osaka 536-8577, Japan.

出版信息

J Phys Condens Matter. 2014 Sep 3;26(35):355005. doi: 10.1088/0953-8984/26/35/355005. Epub 2014 Jul 31.

Abstract

Using density-functional theory calculations combined with recent local-energy and local-stress schemes, we studied the effects of Si segregation on the structural, mechanical and magnetic properties of the Σ3(1 1 1) and Σ11(3 3 2) Fe GBs formed by rotation around the [1 1 0] axis. The segregation mechanism was analyzed by the local-energy decomposition of the segregation energy, where the segregation energy is expressed as a sum of the following four terms: the local-energy change of Si atoms from the isolated state in bulk Fe to the GB segregated state, the stabilization of replaced Fe atoms from the GB to the bulk, the local-energy change of neighboring Fe atoms from the pure GB to the segregated GB and the local-energy change of neighboring Fe atoms from the system of an isolated Si atom in the bulk Fe to the pure bulk Fe. The segregation energy and value of each term greatly depends on the segregation site and Si concentration. The segregation at interface Fe sites with higher local energies in the original GB configurations naturally leads to higher segregation-energy gains, while interface sites with lower local energies can lead to larger energy gains if stronger Si-Fe interactions occur locally in the final segregated configurations. The high Si concentration reduces the segregation-energy gain per Si atom due to the local-energy increases of Si atoms neighboring to each other or through the reduction in the number of stabilized Fe atoms per Si atom as observed in a Si dimer in bulk Fe. In the Si-segregated GBs, Si-Fe bonds enhance local Young's moduli and tend to suppress the interface weakening, while the GB adhesion is slightly reduced. And Fe atoms contacting Si atoms have reduced magnetic moments, due to Si-Fe sp-d hybridization interactions.

摘要

利用密度泛函理论计算并结合最近的局域能量和局域应力方案,我们研究了 Si 偏析对通过绕[1 1 0]轴旋转形成的Σ3(1 1 1)和Σ11(3 3 2)Fe 晶界的结构、力学和磁性质的影响。通过偏析能的局域能量分解来分析偏析机制,其中偏析能表示为以下四项之和:Si 原子从体相 Fe 中的孤立状态到晶界偏析状态的局域能量变化、被取代的 Fe 原子从晶界到体相的稳定化、邻近 Fe 原子从纯晶界到偏析晶界的局域能量变化以及邻近 Fe 原子从体相内孤立 Si 原子的系统到纯体相 Fe 的局域能量变化。偏析能和每项的价值在很大程度上取决于偏析位置和 Si 浓度。在原始晶界构型中具有较高局域能量的界面 Fe 位置的偏析自然会导致更高的偏析能增益,而具有较低局域能量的界面位置如果在最终偏析构型中局部发生更强的 Si-Fe 相互作用,则可以获得更大的能量增益。高 Si 浓度会由于相邻 Si 原子的局域能量增加或由于 Si 原子与每个 Si 原子稳定化的 Fe 原子数量减少而降低每个 Si 原子的偏析能增益,就像在体相 Fe 中的 Si 二聚体中观察到的那样。在 Si 偏析晶界中,Si-Fe 键增强了局部杨氏模量,并倾向于抑制界面弱化,而晶界附着力略有降低。与 Si 原子接触的 Fe 原子的磁矩减小,这是由于 Si-Fe sp-d 杂化相互作用。

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