arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 0706.1012cond-mat.mtrl-scicond-mat.str-el
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用相共存法计算钼的从头算熔化曲线

Ab initio melting curve of molybdenum by the phase coexistence method

C. Cazorla, M. J. Gillan, S. Taioli, D. Alfè

摘要:

我们报告从头计算的熔化曲线的压力范围为0-400 GPa的钼。计算采用密度泛函理论(DFT)与Perdew-Burke-Ernzerhof交换相关功能的投影增强波(PAW)的实现。我们目前的测试表明,这些技术准确地再现实验数据的低温b.c.c.莫,PAW同意密切从全电位线性增广平面波实现的结果。这项工作试图克服固有的不确定性,在早期的DFT计算的熔化曲线的钼,通过使用“参考共存”的技术来确定熔化曲线。在这项技术中,一个经验的参考模型(这里,嵌入原子模型)是准确地拟合DFT分子动力学数据的液体和高温固体,熔融曲线的参考模型是由模拟共存的固体和液体,并通过应用自由能修正的从头计算熔融曲线。计算得到的熔化曲线与常压下的实验结果吻合较好,与高压下的冲击数据吻合较好,但与静态压缩实验得到的高压熔化曲线不一致。径向分布函数的计算结果表明,液体的短程原子有序与高温固体的短程原子有序非常相似,但从固体到液体的过程中,配位数略有降低。在这两个阶段的电子态密度显示只有很小的差异。结果不支持最近的理论,根据该理论,b.c.c.预期dTm/dP值非常低。过渡金属,因为电子在s-p和d态之间重新分布。

英文摘要:

We report ab initio calculations of the melting curve of molybdenum for the pressure range 0-400 GPa. The calculations employ density functional theory (DFT) with the Perdew-Burke-Ernzerhof exchange-correlation functional in the projector augmented wave (PAW) implementation. We present tests showing that these techniques accurately reproduce experimental data on low-temperature b.c.c. Mo, and that PAW agrees closely with results from the full-potential linearized augmented plane-wave implementation. The work attempts to overcome the uncertainties inherent in earlier DFT calculations of the melting curve of Mo, by using the ``reference coexistence'' technique to determine the melting curve. In this technique, an empirical reference model (here, the embedded-atom model) is accurately fitted to DFT molecular dynamics data on the liquid and the high-temperature solid, the melting curve of the reference model is determined by simulations of coexisting solid and liquid, and the ab initio melting curve is obtained by applying free-energy corrections. Our calculated melting curve agrees well with experiment at ambient pressure and is consistent with shock data at high pressure, but does not agree with the high pressure melting curve deduced from static compression experiments. Calculated results for the radial distribution function show that the short-range atomic order of the liquid is very similar to that of the high-T solid, with a slight decrease of coordination number on passing from solid to liquid. The electronic densities of states in the two phases show only small differences. The results do not support a recent theory according to which very low dTm/dP values are expected for b.c.c. transition metals because of electron redistribution between s-p and d states.

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