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arXiv 1302.0062cond-mat.mtrl-sci
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兆巴压力下冷固体氢中质子的经典和量子有序

Classical and quantum ordering of protons in cold solid hydrogen under megabar pressures

Xin-Zheng Li, Brent Walker, Matthew I. J. Probert, Chris J. Pickard, Richard J. Needs, Angelos Michaelides

摘要:

本文采用多种理论方法,从原子水平上研究了冷高压固态氢中质子的经典和量子有序,主要研究氢的第二和第三相,探索量子核运动对这些相的某些特征的影响(通过在相图上的特定点处的多个从头算路径积分分子动力学(PIMD)模拟)。我们还研究了范德华力在这个系统中的重要性,通过使用optB 88-vdW密度泛函,它占非本地相关性进行计算。我们的计算表明,相I和II之间的过渡是强量子性质,由于各向异性间的竞争,限制分子旋转的分子相互作用和促进分子旋转的核位置的热加量子涨落。从相II到III的转变更经典,因为量子核运动只起次要作用,并且转变主要由基本的势能面。用PIMD方法计算了在有限温度下含有24个原子的P21 c对称性结构,发现在非谐量子振动作用下,该结构是稳定的.这种结构给出了一个很好的帐户的红外(IR)和拉曼振子频率相II。我们发现广告支持C2/c结构作为第三阶段的强有力的候选者,因为它仍然是透明的高达300 GPa,即使当量子核效应。最后,我们发现,占范德华力提高了实验和理论之间的协议所考虑的相图的部分,相比以前的工作,采用广泛使用的Perdew-Burke-Ernzerhof(PBE)交换相关功能。

英文摘要:

A combination of state-of-the-art theoretical methods has been used to obtain an atomic-level picture of classical and quantum ordering of protons in cold high-pressure solid hydro-gen. We focus mostly on phases II and III of hydrogen, exploring the effects of quantum nuclear motion on certain features of these phases (through a number of ab initio path-integral molecular dynamics (PIMD) simulations at particular points on the phase diagram). We also examine the importance of van der Waals forces in this system by performing calculations using the optB88-vdW density functional, which accounts for non-local correlations. Our calculations reveal that the transition between phases I and II is strongly quantum in nature, resulting from a competition between anisotropic inter-molecular interactions that restrict molecular rotation and thermal plus quantum fluctuations of the nuclear positions that facilitate it. The transition from phase II to III is more classical because quantum nuclear motion plays only a secondary role and the transition is determined primarily by the underlying potential energy surface. A structure of P21c symmetry with 24 atoms in the primitive unit cell is found to be stable when anharmonic quantum nuclear vibrational motion is included at finite temperatures using the PIMD method. This structure gives a good account of the infra-red (IR) and Raman vibron frequencies of phase II. We find ad-ditional support for C2/c structure as a strong candidate for phase III, since it remains transparent up to 300 GPa, even when quantum nuclear effects are included. Finally, we find that accounting for van der Waals forces improves the agreement between experiment and theory for the parts of the phase diagram considered, when compared to previous work which employed the widely-used Perdew-Burke-Ernzerhof (PBE) exchange-correlation functional.

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