高压下FeO2H2He的晶体结构与弹性性质的第一性原理研究

陈浩楠,  熊彦皓,  刘海博,  徐国淼

陈浩楠, 熊彦皓, 刘海博, 徐国淼. 高压下FeO2H2He的晶体结构与弹性性质的第一性原理研究[J]. 高压物理学报. doi: 10.11858/gywlxb.20261111
引用本文: 陈浩楠, 熊彦皓, 刘海博, 徐国淼. 高压下FeO2H2He的晶体结构与弹性性质的第一性原理研究[J]. 高压物理学报. doi: 10.11858/gywlxb.20261111
CHEN Haonan, XIONG Yanhao, LIU Haibo, XU Guomiao. First-Principles Study of the Crystal Structure and Elastic Properties of FeO2H2He under High Pressure[J]. Chinese Journal of High Pressure Physics. doi: 10.11858/gywlxb.20261111
Citation: CHEN Haonan, XIONG Yanhao, LIU Haibo, XU Guomiao. First-Principles Study of the Crystal Structure and Elastic Properties of FeO2H2He under High Pressure[J]. Chinese Journal of High Pressure Physics. doi: 10.11858/gywlxb.20261111

高压下FeO2H2He的晶体结构与弹性性质的第一性原理研究

doi: 10.11858/gywlxb.20261111
基金项目: 西藏大学高层次人才项目(xzdxdr202509);西藏大学研究生“高水平人才培养计划”项目(2026-GSP-S019)
详细信息
    作者简介:

    陈浩楠(2001-),男,硕士研究生,主要从事高温高压下矿物物性研究. E-mail:19904389365@163.com

    通讯作者:

    刘海博(1994-),男,博士,讲师,主要从事高温高压下矿物物性研究.E-mail:liuhaibo@xzu.edu.cn

  • 中图分类号: O521.2

First-Principles Study of the Crystal Structure and Elastic Properties of FeO2H2He under High Pressure

  • 摘要: 洋岛玄武岩中高比值的3He/4He指示地球深部存在原始氦储库,而地球深部的物质组成和波速异常同样也是当前研究的热点。然而,关于地球深部稳定含氦化合物的了解知之甚少。为此,采用基于密度泛函理论的第一性原理方法,系统计算了30~150 GPa压力条件下FeO2H2He的晶体结构和弹性性质。声子色散和弹性常数计算结果表明, FeO2H2He的R3m三方晶系结构在所计算的静态高压条件下表现出良好的局部动力学稳定性和力学稳定性。泊松比与Pugh比分析显示,FeO2H2He在所研究的压力范围内均表现为延性状态。密度和波速特征综合揭示了FeO2H2He具有作为核幔边界附近候选含氦相的可能性,并且可能是解释超低速区(ultra-low velocity zones, ULVZs)波速异常的潜在矿物组成。研究结果丰富了核幔边界的物质组成,为地球深部氦的赋存与分布提供了新的矿物学约束。

     

  • 图  1  FeO2H2He的晶体结构

    Figure  1.  Crystal structure of FeO2H2He

    图  2  FeO2H2He的体积(a)和密度(b)随压力的变化

    Figure  2.  Volume (a) and density (b) of FeO2H2He as a function of pressure

    图  3  不同压力下FeO2H2He的声子色散曲线

    Figure  3.  Phonon dispersion curves of FeO2H2He under different pressures

    图  4  静态条件下FeO2H2He的弹性常数(a)与弹性模量(b)随压力的变化

    Figure  4.  Elastic constants (a) and elastic moduli (b) of FeO2H2He under static conditions as a function of pressure

    图  5  FeO2H2He的弹性各向异性指数(a)和泊松比(b)随压力的变化

    Figure  5.  Universal elastic anisotropy index (a) and Poisson's ratio (b) of FeO2H2He as a function of pressure

    图  6  FeO2H2He的密度(a)和波速(b)随深度的变化

    Figure  6.  Density (a) and wave velocity (b) of FeO2H2He as a function of depth

    表  1  135 GPa下不同矿物(模型)的波速和密度对比

    Table  1.   Comparison of wave velocity and density of different minerals (model) at 135 GPa

    Minerals/model vS/(km·s−1) vP/(km·s−1) ρ/(g·cm−3) vP/vS Ref.
    FeO2 6.05 11.74 7.66 1.94 [21]
    FeO2He 7.27 13.02 7.56 1.79 [21]
    PREM ~6.5 ~13.0 ~5.6 ~2.0 [30]
    FeO2H2He 5.08 11.23 5.78 2.21 This study
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  • 收稿日期:  2026-06-08
  • 修回日期:  2026-08-30
  • 网络出版日期:  2026-09-09

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