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Diabatic-At-Construction Method for Diabatic and Adiabatic Ground and Excited States Based on Multistate Density Functional Theory

机译:基于多态密度泛函理论的绝热绝热基态和激发态的绝热构造方法

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摘要

We describe a diabatic-at-construction (DAC) strategy for defining diabatic states to determine the adiabatic ground and excited electronic states and their potential energy surfaces using the multistate density functional theory (MSDFT). The DAC approach differs in two fundamental ways from the adiabatic-to-diabatic (ATD) procedures that transform a set of preselected adiabatic electronic states to a new representation. (1) The DAC states are defined in the first computation step to form an active space, whose configuration interaction produces the adiabatic ground and excited states in the second step of MSDFT. Thus, they do not result from a similarity transformation of the adiabatic states as in the ATD procedure; they are the basis for producing the adiabatic states. The appropriateness and completeness of the DAC active space can be validated by comparison with experimental observables of the ground and excited states. (2) The DAC diabatic states are defined using the valence bond characters of the asymptotic dissociation limits of the adiabatic states of interest, and they are strictly maintained at all molecular geometries. Consequently, DAC diabatic states have specific and well-defined physical and chemical meanings that can be used for understanding the nature of the adiabatic states and their energetic components. Here we present results for the four lowest singlet states of LiH and compare them to a well-tested ATD diabatization method, namely the 3-fold way; the comparison reveals both similarities and differences between the ATD diabatic states and the orthogonalized DAC diabatic states. Furthermore, MSDFT can provide a quantitative description of the ground and excited states for LiH with multiple strongly and weakly avoided curve crossings spanning over 10 Å of interatomic separation.
机译:我们描述了一种用于定义绝热状态的绝热构造(DAC)策略,以使用多态密度泛函理论(MSDFT)确定绝热基态和激发电子态及其势能面。 DAC的方法从绝热到绝热(ATD)程序的两个基本方式不同,该程序将一组预选的绝热电子状态转换为新的表示形式。 (1)在第一个计算步骤中定义DAC状态以形成一个活动空间,其配置相互作用在MSDFT的第二个步骤中产生绝热基态和激发态。因此,它们不是像ATD程序那样由绝热状态的相似性转换产生的;它们是产生绝热状态的基础。通过与基态和激发态的实验观测值进行比较,可以验证DAC活动空间的适当性和完整性。 (2)DAC绝热态是使用感兴趣的绝热态的渐近解离极限的价键特征来定义的,并且在所有分子几何结构中均严格保持它们的价态。因此,DAC绝热态具有特定且定义明确的物理和化学含义,可用于理解绝热态及其能量成分的性质。在这里,我们给出LiH的四个最低单重态的结果,并将它们与经过充分测试的ATD绝热方法进行比较,即3折法。比较结果显示了ATD非绝热态与正交DAC非绝热态之间的异同。此外,MSDFT可以定量描述LiH的基态和激发态,并避免了跨越原子间间距超过10Å的多个强而弱的曲线交叉。

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