论文标题
镁的熔融曲线从依从算分子动力学模拟最高460 GPA
Melting curve of magnesium up to 460 GPa from ab initio molecular dynamics simulations
论文作者
论文摘要
基于从头算分子动力学模拟,我们使用固液并存方法确定了镁(MG)的熔融曲线,最高〜460 GPA。在〜30至100 GPA之间,我们的熔融曲线明显低于静态实验的曲线,但与最近的冲击实验非常吻合。最多约450 GPA,我们的熔融曲线通常与使用小细胞共存方法的第一原理计算中的熔点一致。我们发现,在几百个GPA的高压下,由于液相中原子间相互作用的强烈软化,MG的固定液并存模拟显示出与其他金属系统(如铝)明显不同的特征。例如,在给定的体积时,保持稳定的固定液并存状态的压力和温度范围可能很小。液相的强烈软化也会导致重入融化的异常行为在很高的压力下发生。从〜305 GPA预测,返回熔点的发作接近于小细胞共存方法的300 GPA。我们表明,考虑到重入融化的计算熔点可以很好地适合低阶Kechin方程,从而使我们有可能在第一次以高于50 GPA的压力下获得MG的第一原理熔化曲线。对于其他在高压下液相软化的系统,固定液并存模拟以及重新进入的融化也有类似的特征。
Based on ab initio molecular dynamics simulations, we determined the melting curve of magnesium (Mg) up to ~460 GPa using the solid-liquid coexistence method. Between ~30 and 100 GPa, our melting curve is noticeably lower than those from static experiments, but is in good agreement with recent shock experiments. Up to ~450 GPa, our melting curve is generally consistent with the melting points from first-principles calculations using the small-cell coexistence method. We found that, at high pressures of a few hundred GPa, due to the strong softening of interatomic interactions in the liquid phase, solid-liquid coexistence simulations of Mg show some characteristics distinctively different from other metal systems, such as aluminum. For example, at a given volume, the pressure and temperature range for maintaining a stable solid-liquid coexistence state can be very small. The strong softening in the liquid phase also causes the unusual behavior of reentrant melting to occur at very high pressures. The onset of reentrant melting is predicted at ~305 GPa, close to that at ~300 GPa from the small-cell coexistence method. We show that the calculated melting points, considering reentrant melting, can be excellently fitted to a low-order Kechin equation, thereby making it possible for us to obtain a first-principles melting curve of Mg at pressures above 50 GPa for the first time. Similar characteristics in solid-liquid coexistence simulations, as well as reentrant melting, are also expected for other systems with strong softening in the liquid phase at high pressures.