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Quantum mechanical calculation of diffusion of hydrogen isotopes in vanadium

机译:钒中氢同位素扩散的量子力学计算

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摘要

Diffusion of hydrogen isotopes in vanadium was investigated by a quantum mechanical calculation. Wave functions and the corresponding eigen energies (ξ) for hydrogen isotopes were obtained as a function of hydrogen position along the diffusion path (ξ) by solving the three dimensional Schrodinger equation. Hydrogen potential was calculated by using a first principles method with a nudged elastic band technique. By analyzing the E-ξ curves, the tunneling matrix elements were obtained for the coincidence states between two neighboring tetrahedral sites. It was clarified that the tunneling between ground states was dominant at low temperatures, whereas the contribution of that between the first exited states becomes larger at higher temperatures. The transition temperature of the dominant tunneling decreases with the isotope mass. The calculated temperature dependence of the diffusion for the V-H system quantitatively agreed with the experimental data in the literature, although those for the V-D and -T systems were somewhat underestimated.
机译:通过量子力学计算研究了氢同位素在钒中的扩散。通过求解三维薛定inger方程,获得了氢同位素的波函数和相应的本征能(ξ),作为氢沿扩散路径(ξ)的位置的函数。氢势通过使用带微动弹性带技术的第一原理方法来计算。通过分析E-ξ曲线,获得了两个相邻四面体位点之间的重合状态的隧穿矩阵元素。明确了在低温下基态之间的隧穿占主导地位,而在较高温度下第一个出口态之间的隧穿贡献更大。主导隧穿的转变温度随同位素质量而降低。尽管对于V-D和-T系统的扩散被低估了,但对于V-H系统的扩散所计算的温度依从性在数量上与文献中的实验数据一致。

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