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Structural and vibrational properties of lithium under ambient conditions within density functional theory

机译:密度函数理论内环境条件下锂的结构和振动性质

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We apply a general first-principles approach to derive the phase diagram of metallic lithium at ambient pressure between 0 and 350 K, including identification of candidate phases. We use ab initio random structure searching to identify competing phases and supplement the results with calculations of vibrational properties and relevant derived neutron diffraction patterns. Strong quantum nuclear effects are present, prompting a careful treatment of vibrations. We directly map the Born-Oppenheimer surface of Li, allowing the extension of the normal quasi-harmonic treatment of vibrations to a "quasi-anharmonic" approach, where the effects of anharmonicity are included. The Gibbs free energies of the fcc, bcc, hcp, and 9R phases are derived using a variety of equations of state. We find that the anharmonic contribution to the Gibbs free energies of Li phases is of the same order as the differences between phases. Anharmonicity also makes a noticeable difference to the 0-K phonon dispersion of the bcc phase, with the largest difference at the N-point phonon. The ordering of phase transitions that we find agrees with the calculations of Ackland et al. [Science 356, 1254 (2017)], even when anharmonic effects are included, suggesting that a quasi-harmonic treatment is sufficient for correct phase behavior. We show explicitly that the martensitic phase transition from close-packed to bcc lithium upon heating is driven by entropic contributions to the phonon free energy.
机译:我们应用一般的一般性原则方法来导出在0和350k之间的环境压力下的金属锂相图,包括鉴别候选阶段。我们使用AB Initio随机结构搜索来识别竞争阶段,并补充结果,并通过计算振动性能和相关的衍生中子衍射图案来补充结果。存在强烈的量子核效应,促使仔细治疗振动。我们直接映射LI的出生对立海米表面,允许延长振动的正常准谐波处理,以“准无谐波”方法,包括厌氧性的影响。使用各种状态方程来源的FCC,BCC,HCP和9R相的GIBBS自由能量。我们发现对李阶段的Gibbs自由能量的anharmonic贡献与阶段之间的差异相同。 Anharmonicity还对BCC阶段的0-K个声子分散差异有明显的差异,具有n点声位的最大差异。我们发现的阶段转换的排序与Ackland等人的计算同意。 [Science 356,1254(2017)],即使包括厌氧效应,表明准谐波处理足以用于正确的相位行为。我们明确地显示了在加热时从紧密包装到BCC锂的马氏体相转变由熵对自由能量的熵贡献驱动。

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