2008
DOI: 10.1016/j.commatsci.2007.10.010
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Glass formation and local structure evolution in rapidly cooled Pd55Ni45 alloy melt: Molecular dynamics simulation

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Cited by 14 publications
(9 citation statements)
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“…Finally, the fourth integer (l) is needed to difference between the cases if the first three indices are the same but the bond geometries are different. The 1551, 1431, 1541, 1321 bonded pairs are represent amorphous-type bonded pairs, while 1421, 1422, 1441 and 1661 bonded pairs predominant in the crystal phase [33].…”
Section: The Honeycutt-andersen (Ha) Methodsmentioning
confidence: 99%
“…Finally, the fourth integer (l) is needed to difference between the cases if the first three indices are the same but the bond geometries are different. The 1551, 1431, 1541, 1321 bonded pairs are represent amorphous-type bonded pairs, while 1421, 1422, 1441 and 1661 bonded pairs predominant in the crystal phase [33].…”
Section: The Honeycutt-andersen (Ha) Methodsmentioning
confidence: 99%
“…The 1421 and 1422 bonded pairs are characteristic bonded pairs for FCC and HCP crystal structures, respectively. The 1661 and 1441 bonded pairs are the characteristic bonded pairs for BCC crystal structure [32]. The pair fractions shown here are normalised so that the sum over all cases for the nearest neighbours is summed to unity.…”
Section: Methods Of Structural Analysismentioning
confidence: 99%
“…1. 引言 在凝固过程中,合金的显微形貌很大程度上受到 成分和冷却条件的影响 [1,2] 。 现有的许多凝固理论都是 基于实验方法所提供的结果而产生的 [3,4] 。但是,在快 速冷却后得到的非晶组织,其晶化后的组织形貌可能 发生什么变化还很少被涉及。 由于实验条件的限制,极端条件下的材料组织结 构很难获得。在这些条件下,采用数值模拟的方法就 有很大的优势。在这一领域,分子动力学模拟(MD) 的方法已经广泛的应用于快速凝固非晶形成及其晶 化过程研究 [5,6] 。Ag-Cu 纳米材料的导电、催化和杀菌 作用具有广泛的用途 [7][8][9] , 特别是非平衡条件下获得的 纳米和非晶结构,更有利于发挥其性能。Ag-Cu 合金 中原子半径之比为 1.13,根据非晶态形成的尺寸效应 [10] ,凝固过程中 Ag-Cu 容易形成非晶态结构。目前, Maxwell-Boltzmann 分布。在模拟中采用恒压恒温的 分子动力学方法(NPT)。由 Nose-Hoover [11,12] 方法控制 系统的温度和压力,并运用 Velocity-Verlet 算法 [13] [14,15] ,在…”
Section: Ag-unclassified