含时密度泛函理论及应用的最新发展

覃睿

覃睿. 含时密度泛函理论及应用的最新发展[J]. 高压物理学报, 2019, 33(3): 030101. doi: 10.11858/gywlxb.20190747
引用本文: 覃睿. 含时密度泛函理论及应用的最新发展[J]. 高压物理学报, 2019, 33(3): 030101. doi: 10.11858/gywlxb.20190747
QIN Rui. New Developments of Time-Dependent Density Functional Theory and Its Applications[J]. Chinese Journal of High Pressure Physics, 2019, 33(3): 030101. doi: 10.11858/gywlxb.20190747
Citation: QIN Rui. New Developments of Time-Dependent Density Functional Theory and Its Applications[J]. Chinese Journal of High Pressure Physics, 2019, 33(3): 030101. doi: 10.11858/gywlxb.20190747

含时密度泛函理论及应用的最新发展

doi: 10.11858/gywlxb.20190747
详细信息
    作者简介:

    覃 睿(1982-),男,博士,副研究员,主要从事计算材料研究. E-mail:qinrui@caep.cn

  • 中图分类号: O521.2

New Developments of Time-Dependent Density Functional Theory and Its Applications

  • 摘要: 密度泛函理论在材料计算研究领域得到了广泛的应用,然而它无法处理含时问题和材料的激发态性质。Runge-Gross定理奠定了含时密度泛函理论的基础,为研究这两类问题提供了有效的手段。经过三十多年的发展,含时密度泛函已被应用到量子化学、材料计算等多个领域,人们也更加了解其优势和不足。目前,含时密度泛函理论和方法仍在迅速发展。本文简要回顾含时密度泛函方法的发展历史,介绍近年来含时密度泛函在理论和应用方面的一些重要进展,总结当前在含时密度泛函领域存在的重要难题以及面临的挑战,展望其发展方向和趋势。

     

  • 图  对CO2分子的TDDFT研究(上图为偶极矩随时间演化,下图为通过傅里叶变换得到的谱(实线)与通过线性响应得到的谱(虚线)的比较)[23]

    Figure  1.  TDDFT calculation for the CO2 molecule (Top: time-dependent dipole moment. Bottom: dipole spectrum (full line) by Fourier transformation of dipole moment, compared with spectrum from LR-TDDFT (thin line).)[23]

    图  乙炔在17.5 eV激光脉冲激发下的含时电子局域函数(TDELF)变化的快照[28]

    Figure  2.  Snapshots of the time-dependent electron localization function (TDELF) for the excitation of acetylene by a 17.5 eV laser pulse[28]

    图  偶极近似破坏了晶体哈密顿量的空间周期性

    Figure  3.  Spatial periodicity of the Hamiltonian destroyed by the dipole approximation

    图  块材硅的光吸收谱的RPA、TDDFT-ALDA计算和实验对比[73]

    Figure  4.  Optical absorption spectrum of bulk Si: RPA, TDDFT-ALDA calculations and experiment[73]

    图  采用bootstrap交换关联核的TDDFT计算各类半导体块材的光吸收谱及其与RPA计算、实验结果的对比[74]

    Figure  5.  Optical absorption spectra of various bulk semiconductors calculated with TDDFT using the bootstrap xc kernel compared with the RPA calculations and experiments[74]

    图  沿${\varGamma X}$${\varGamma L}$方向的块材硅的高次谐波谱以及对应的联合态密度(JDOS) [76]

    Figure  6.  High harmonic spectra for the ${\varGamma X}$ polarization direction (red line) and the ${\varGamma L}$ direction (blue line); the bottom panel shows the corresponding joint density of states (JDOS) [76]

    图  计算得到的价电子动态结构因子与Sperling实验测量谱的对比[7879]

    Figure  7.  Calculated dynamic structure factor of valence electrons compared with the measured spectrum of Sperling et al. [7879]

    表  1  一些气相Ar-TCNE体系的激发能E(单位eV)和振动强度f的计算和实验对比[57]

    Table  1.   Excitation energies E (eV) and oscillator strengths f of several gas phase Ar-TCNE systems: theory and experiment[57]

    Ar B3LYP BNL ($\gamma $=0.5) BNL $\gamma^* $ Exp.[27]
    E f E $\gamma^* $ E f E f
    Benzene 2.1 0.03 4.4 0.33 3.8 0.03 3.59 0.02
    Toluene 1.8 0.04 4.0 0.32 3.4 0.03 3.36 0.03
    O-xylene 1.5 0 3.7 0.31 3.0 0.01 3.15 0.05
    Naphthalene 0.9 0 3.3 0.32 2.7 0 2.60 0.01
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