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首页> 外文期刊>Journal of chemical theory and computation: JCTC >Peak-Shifting in Real-Time Time-Dependent Density Functional Theory
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Peak-Shifting in Real-Time Time-Dependent Density Functional Theory

机译:实时时变密度泛函理论中的峰移

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In recent years, the development and application of real-time time-dependent density functional theory (RT-TDDFT) has gained momentum as a computationally efficient method for modeling electron dynamics and properties that require going beyond a linear response of the electron density. However, the RT-TDDFT method within the adiabatic approximation can unphysically shift absorption peaks throughout the electron dynamics. Here, we investigate the origin of these time-dependent resonances observed in RT-TDDFT spectra. Using both exact exchange and hybrid exchange-correlation approximate functionals, adiabatic RT-TDDFT gives time-dependent absorption spectra in which the peaks shift in energy as populations of the excited states fluctuate, while exact wave function methods yield peaks that are constant in energy but vary in intensity. The magnitude of the RT-TDDFT peak shift depends on the frequency and intensity of the applied field, in line with previous studies, but it oscillates as a function of time-dependent molecular orbital populations, consistent with a time-dependent superposition electron density. For the first time, we provide a rationale for the direction and magnitude of the time-dependent peak shifts based on the molecular electronic structure. For three small molecules, H-2, HeH+, and LiH, we give contrasting examples of peak-shifting to both higher and lower energies. The shifting is explained as coupled one-electron transitions to a higher and a lower lying state. Whether the peak shifts to higher or lower energies depends on the relative energetics of these one-electron transitions.
机译:近年来,实时时变密度泛函理论(RT-TDDFT)的发展和应用已成为一种势头强劲的计算方法,可用于对电子动力学和特性建模,该模型需要超越电子密度的线性响应。但是,绝热近似中的RT-TDDFT方法会在整个电子动力学过程中非物理地移动吸收峰。在这里,我们调查在RT-TDDFT光谱中观察到的这些与时间有关的共振的起源。绝热RT-TDDFT同时使用精确交换和混合交换相关近似函数,给出了随时间变化的吸收光谱,其中随着激发态总体的波动,峰的能量发生位移,而精确的波函数方法产生的峰在能量上恒定,但是强度不同。与先前的研究一致,RT-TDDFT峰位移的大小取决于所施加场的频率和强度,但它随时间变化的分子轨道总体而变化,与时间变化的叠加电子密度一致。首次,我们基于分子电子结构为时间依赖性峰位移的方向和大小提供了理论依据。对于H-2,HeH +和LiH这三个小分子,我们给出了将峰移至较高和较低能量的对比示例。将该位移解释为耦合的单电子跃迁到较高和较低的躺卧状态。峰是转移到较高还是较低的能量取决于这些单电子跃迁的相对能量。

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