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What Is the Accuracy Limit of Adiabatic Linear-Response TDDFT Using Exact Exchange-Correlation Potentials and Approximate Kernels?

机译:使用精确的交换相关电位和近似内核的绝热线性响应TDDFT的精度极限是多少?

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Calculation of vertical excitation energies by the adiabatic linear-response time-dependent density-functional theory (TDDFT) requires static Kohn-Sham potentials and exchange-correlation kernels. When these quantities are derived from standard density-functional approximations DFA), mean absolute errors (MAE) of the method are known to range from 0.2 eV to over 1 eV, depending on the functional and type of excitation. We investigate how the performance of TDDFT varies when increasingly accurate exchange-correlation potentials derived from Hartree-Fock HF) and post-HF wavefunctions are combined with different approximate kernels. The lowest MAEs obtained in this manner for valence excitations are about 0.15-0.2 eV, which appears to be the practical limit of the accuracy of TDDFT that can be achieved by improving the Kohn-Sham potentials alone. These findings are consistent with previous reports on the benefits of accurate exchange-correlation potentials in TDDFT, but provide new insights and afford more definitive conclusions.
机译:通过绝热线性响应时间依赖性密度 - 功能理论(TDDFT)计算垂直激励能量需要静态Kohn-Sham电位和交换相关性核。当这些数量来自标准密度 - 官能近似DFA时,该方法的平均绝对误差(MAE)被已知为0.2eV至超过1eV,这取决于激发的功能和类型。我们调查如何在从Hartree-Fock HF衍生的越来越准确的交换相关电位时变化的TDDFT的性能如何)和HF波力发射与不同的近似核相结合。以这种价值激发以这种方式获得的最低MAE约为0.15-0.2eV,这似乎是通过改善单独的Kohn-Sham潜力来实现的TDDFT精度的实际限制。这些发现与先前关于TDDFT中准确交换相关电位的好处的报告一致,但提供了新的见解并提供了更明确的结论。

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