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首页> 外文期刊>Nuclear instruments and methods in physics research >Migration behaviors of helium atoms near tungsten surfaces: A molecular dynamics study
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Migration behaviors of helium atoms near tungsten surfaces: A molecular dynamics study

机译:钨表面附近氦原子的迁移行为:分子动力学研究

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Under the fusion environment, the behavior of helium atoms near tungsten (W) surfaces plays a crucial role in surface morphological evolution and near-surface structural evolution of tungsten. In this paper, the migration behaviors of single helium atoms near W (2 1 1) and W (3 1 1) surfaces were investigated using molecular dynamics simulations. The results show that these single atoms can be well-described by the theory of continuous diffusion of particles in a semi-infinite medium, and different types of trap mutations occur for both surfaces. Although the temperature has an impotent impact on the occurrence probabilities of different types of trap mutations and the probabilities of helium atoms escaping from trap sites, there is no a strict relationship between the depth and temperature for trap mutations occurring. For the W (2 1 1) surface, an approximately one-dimensional diffusion may take place along the 1 1 1 directions when the helium atoms are trapped near 2 layers below the W surface. For the W (3 1 1) surface, the behaviors of trap mutations seem more significant than (2 1 1) and (1 1 1) surfaces at T = 1000 K. To investigate the diffusion and trap mutation processes, the nudged elastic band (NEB) method was also applied. These results can be helpful for understanding of helium release, helium retention, subsurface helium clustering, as well as surface morphological evolution.
机译:在聚变环境下,钨表面附近氦原子的行为在钨的表面形态演化和近表面结构演化中起着至关重要的作用。在本文中,使用分子动力学模拟研究了单氦原子在W(2 1 1)和W(3 1 1)表面附近的迁移行为。结果表明,这些单原子可以用半无限介质中粒子的连续扩散理论很好地描述,并且两个表面都发生不同类型的陷阱突变。尽管温度对不同类型的陷阱突变的发生概率以及从陷阱位点逸出的氦原子的概率影响不大,但是在深度和温度之间对于陷阱突变的发生并不存在严格的关系。对于W(2 1 1)表面,当氦原子被困在W表面以下2层附近时,沿<1 1 1>方向可能发生一维扩散。对于W(3 1 1)表面,在T = 1000 K时,陷阱突变的行为似乎比(2 1 1)和(1 1 1)表面更为显着。要研究扩散和陷阱突变的过程,请轻推弹性带(NEB)方法也被应用。这些结果有助于理解氦的释放,氦的截留,地下氦的聚集以及表面形态的演变。

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