氧化锌的高压电子结构、光学性质与电性能的理论研究

李凡生 余小英 张飞鹏 彭金云 房慧 张忻

李凡生, 余小英, 张飞鹏, 彭金云, 房慧, 张忻. 氧化锌的高压电子结构、光学性质与电性能的理论研究[J]. 高压物理学报, 2016, 30(2): 101-108. doi: 10.11858/gywlxb.2016.02.003
引用本文: 李凡生, 余小英, 张飞鹏, 彭金云, 房慧, 张忻. 氧化锌的高压电子结构、光学性质与电性能的理论研究[J]. 高压物理学报, 2016, 30(2): 101-108. doi: 10.11858/gywlxb.2016.02.003
LI Fan-Sheng, YU Xiao-Ying, ZHANG Fei-Peng, PENG Jin-Yun, FANG Hui, ZHANG Xin. Theoretical Investigation on Electronic Structure, Optical Properties and Electrical Properties of Zinc Oxide under High Pressure[J]. Chinese Journal of High Pressure Physics, 2016, 30(2): 101-108. doi: 10.11858/gywlxb.2016.02.003
Citation: LI Fan-Sheng, YU Xiao-Ying, ZHANG Fei-Peng, PENG Jin-Yun, FANG Hui, ZHANG Xin. Theoretical Investigation on Electronic Structure, Optical Properties and Electrical Properties of Zinc Oxide under High Pressure[J]. Chinese Journal of High Pressure Physics, 2016, 30(2): 101-108. doi: 10.11858/gywlxb.2016.02.003

氧化锌的高压电子结构、光学性质与电性能的理论研究

doi: 10.11858/gywlxb.2016.02.003
基金项目: 

国家自然科学基金 11347141

国家自然科学基金 21465004

国家自然科学基金 51572066

广西民族师范学院人才科研启动项目 2014RCDT002

广西民族师范学院博士科研启动项目 2013RCBS001

广西高等学校科学技术研究项目 2013YB268

详细信息
    作者简介:

    李凡生(1974—), 男,硕士,副教授,主要从事凝聚态物理及实验方面研究.E-mail:453291572@qq.com

    通讯作者:

    余小英(1972—), 女,硕士,副教授,主要从事计算物理和物理实验方面研究.E-mail:414269867@qq.com

  • 中图分类号: O521.2;O649

Theoretical Investigation on Electronic Structure, Optical Properties and Electrical Properties of Zinc Oxide under High Pressure

  • 摘要: 基于密度泛函理论从头计算法, 研究了500 GPa外压力条件下纤锌矿结构ZnO氧化物的晶格结构、电子结构、光学性质和导电性能。计算分析结果表明,在500 GPa外压力下,ZnO氧化物的晶格对称性保持不变,晶格参数减小,Zn—O键长和O—Zn—O键角均减小,但不同方向上材料的可压缩性不同;ZnO氧化物的带隙类型仍为直接带隙,其宽度增加到1.65 eV;费米能级附近的能级数量减少,态密度降低,电子在不同能量区域的局域化趋势明显;ZnO氧化物的光吸收向高能量范围扩展,低能量光学吸收降低,高能量光吸收增强。分析结果表明,500 GPa的外压力下,ZnO氧化物费米能级附近的载流子浓度、有效质量和迁移速率均降低,其电性能降低。

     

  • 图  ZnO晶体结构三维示意图

    Figure  1.  3D Schematic of crystal structure of ZnO

    图  ZnO氧化物键长和键角示意图

    Figure  2.  Schematic of the bond length and bond angle for ZnO oxides

    图  500 GPa压力下ZnO氧化物的键长和键角

    Figure  3.  Bond lengths and bond angles for ZnO oxides under 500 GPa pressure

    图  计算所得无压力下和500 GPa压力下ZnO氧化物的能带结构

    Figure  4.  Calculated band structures for ZnO oxides under 0 and 500 GPa pressure

    图  计算所得无压力和500 GPa压力下ZnO氧化物的态密度

    Figure  5.  Calculated density of states for ZnO oxides under 0 and 500 GPa pressure

    图  计算所得无压力和500 GPa压力下ZnO氧化物的分态密度

    Figure  6.  Calculated partial density of states for ZnO oxides under 0 and 500 GPa pressure

    图  计算所得无压力和500 GPa压力下ZnO氧化物的介电函数

    Figure  7.  Calculated dielectric functions for ZnO oxides under 0 and 500 GPa pressure

    表  1  不同压力条件下ZnO的晶格参数

    Table  1.   Lattice parameters of ZnO at different pressures

    Pressure/
    (GPa)
    a/(nm)b/(nm)c/(nm)
    00.330 980.330 980.530 54
    5000.220 380.220 380.535 18
    Pressure/
    (GPa)
    α/(°)β/(°)γ/(°)Space
    group
    0
    500
    9090120P63mc
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  • 收稿日期:  2015-04-07
  • 修回日期:  2015-04-30

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