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通过从头算模拟得到的KCaF和NaMgF的相图。

The phase diagrams of KCaF and NaMgF by ab initio simulations.

作者信息

Jakymiw Clément, Vočadlo Lidunka, Dobson David P, Bailey Edward, Thomson Andrew R, Brodholt John P, Wood Ian G, Lindsay-Scott Alex

机构信息

1Laboratoire de Géologie de Lyon, Université Claude Bernard Lyon1, Ecole Normale Supérieure de Lyon, 46 allée d'Italie, 69342 Lyon Cedex 07, France.

2Department of Earth Sciences, University College London, Gower Street, London, WC1E 6BT UK.

出版信息

Phys Chem Miner. 2018;45(4):311-322. doi: 10.1007/s00269-017-0920-3. Epub 2017 Sep 13.

Abstract

ABF compounds have been found to make valuable low-pressure analogues for high-pressure silicate phases that are present in the Earth's deep interior and that may also occur in the interiors of exoplanets. The phase diagrams of two of these materials, KCaF and NaMgF, have been investigated in detail by static ab initio computer simulations based on density functional theory. Six ABF polymorphs were considered, as follows: the orthorhombic perovskite structure (GdFeO-type; space group ); the orthorhombic CaIrO structure (; commonly referred to as the "post-perovskite" structure); the orthorhombic SbS and LaS structures (both ); the hexagonal structure previously suggested in computer simulations of NaMgF (6/); the monoclinic structure found to be intermediate between the perovskite and CaIrO structures in CaRhO (2/). Volumetric and axial equations of state of all phases considered are presented. For KCaF, as expected, the perovskite phase is shown to be the most thermodynamically stable at atmospheric pressure. With increasing pressure, the relative stability of the KCaF phases then follows the sequence: perovskite → LaS structure → SbS structure → 6/ structure; the CaIrO structure is never the most stable form. Above about 2.6 GPa, however, none of the KCaF polymorphs are stable with respect to dissociation into KF and CaF. The possibility that high-pressure KCaF polymorphs might exist metastably at 300 K, or might be stabilised by chemical substitution so as to occur within the standard operating range of a multi-anvil press, is briefly discussed. For NaMgF, the transitions to the high-pressure phases occur at pressures outside the normal range of a multi-anvil press. Two different sequences of transitions had previously been suggested from computer simulations. With increasing pressure, we find that the relative stability of the NaMgF phases follows the sequence: perovskite → CaIrO structure → SbS structure → 6/ structure. However, only the perovskite and CaIrO structures are stable with respect to dissociation into NaF and MgF.

摘要

已发现ABF化合物可成为地球深部内部存在的高压硅酸盐相以及系外行星内部可能出现的高压硅酸盐相的有价值的低压类似物。基于密度泛函理论,通过静态从头算计算机模拟详细研究了其中两种材料KCaF和NaMgF的相图。考虑了六种ABF多晶型物,如下:正交钙钛矿结构(GdFeO型;空间群);正交CaIrO结构(;通常称为“后钙钛矿”结构);正交SbS和LaS结构(均为);先前在NaMgF的计算机模拟中提出的六方结构(6/);在CaRhO(2/)中发现的单斜结构,介于钙钛矿和CaIrO结构之间。给出了所考虑的所有相的体积和轴向状态方程。对于KCaF,正如预期的那样,钙钛矿相在大气压下显示为最热力学稳定的相。随着压力增加,KCaF相的相对稳定性顺序如下:钙钛矿→LaS结构→SbS结构→6/结构;CaIrO结构从未是最稳定的形式。然而,在约2.6 GPa以上,KCaF的任何多晶型物相对于分解为KF和CaF而言都不稳定。简要讨论了高压KCaF多晶型物在300 K下可能亚稳存在,或可能通过化学取代而稳定,从而在多砧压机的标准操作范围内出现的可能性。对于NaMgF,向高压相的转变发生在多砧压机的正常压力范围之外。先前从计算机模拟中提出了两种不同的转变顺序。随着压力增加,我们发现NaMgF相的相对稳定性顺序如下:钙钛矿→CaIrO结构→SbS结构→6/结构。然而,只有钙钛矿和CaIrO结构相对于分解为NaF和MgF而言是稳定的。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/980f/6560713/d6b963e135b2/269_2017_920_Fig1_HTML.jpg

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