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首页> 外文期刊>Philosophical Magazine, A. Physics of condensed matter, defects and mechanical properties >Ab-initio simulation of isolated screw dislocations in bcc Mo and Ta
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Ab-initio simulation of isolated screw dislocations in bcc Mo and Ta

机译:bcc Mo和Ta中孤立的螺旋位错的从头算模拟

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The equilibrium core structure of isolated. (a/2) [111] screw dislocations are calculated using a first-principles pseudopotential plane-wave method within the local-density approximation of density functional theory. The long-range strain field of the dislocation is treated using a variation of the recently developed lattice Green's function boundary condition method. This flexible boundary method allows the dislocation to be contained in a very small simulation cell without compromising the fidelity of the final core configuration. Supercells of 168, 270 and 504 atoms are used to evaluate the local screw and edge displacements of the (a/2) [111] screw dislocation in Mo and Ta. These results are contrasted with previous results from atomistic and dipole array calculations. We rnd that the isolated screw dislocations are evenly spread on three conjugate (110) planes for both Mo and Ta. The twinning-antitwinning anisotropy is calculated in Mo by applying a pure glide stress on the (112) plane. In these simulations the dislocation always moves on a {110} plane. The lattice frictional stress to move a straight screw dislocation on the (112) plane in the antitwinning and twinning sense is estimated at 0.025 mu and 0.0125 mu respectively. This is in good agreement with parallel atomistic simulations and experimental measurements of the slip asymmetry. [References: 23]
机译:隔离的平衡核心结构。 (a / 2)[111]螺钉位错是在密度泛函理论的局部密度近似范围内使用第一原理pseudo势平面波方法计算的。使用最近开发的晶格格林函数边界条件方法的变体来处理位错的远距离应变场。这种灵活的边界方法允许将位错包含在非常小的模拟单元中,而不会影响最终核心配置的保真度。使用168、270和504个原子的超单元来评估Mo和Ta中(a / 2)[111]螺钉位错的局部螺钉和边缘位移。这些结果与原子和偶极子阵列计算的先前结果形成对比。我们发现,对于Mo和Ta,孤立的螺钉位错均匀分布在三个共轭(110)平面上。通过在(112)平面上施加纯滑移应力,可以在Mo中计算孪生-反缠绕各向异性。在这些模拟中,位错始终在{110}平面上移动。在反缠绕和孪生的意义上,使直线螺钉位错在(112)平面上移动的晶格摩擦应力估计分别为0.025μ和0.0125μ。这与滑移不对称的并行原子模拟和实验测量非常吻合。 [参考:23]

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