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Exchange-only optimized effective potential for molecules from resolution-of-the-identify techniques: Comparison with the local density approximation, with and without asymptotic correction

机译:分子识别技术仅可交换的优化有效分子势:与有和无渐近校正的局部密度近似比较

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The optimized effective potential (OEP) is (within a certain linear response approximation) the exact exchange-correlation potential of density-functional theory (DFT). In the program DEMON-DYNARHO, we have implemented the OEP at the exchange-only level without the evaluation of four-center integrals using resolution-of-the-identify techniques. We point out that great care must be taken in treating the asymptotic behavior of the OEP in finite basis set methods. Our results are compared with previous work using OEP-like potentials. Our OEP orbital energies are compared with experimental ionization potentials. Hartree-Fock (HF) orbital energies, and with orbital energies from the local density approximation (LDA) potential, with and without asymptotic correction (AC). We find that OEP orbital energies are a much better approximation to experimental ionization potentials than are HF orbital energies. LDA orbital energies also correlate well with OEP orbital energies, except for a molecule-dependent rigid shift, due to the well-known fact that the LDA potential falls off too rapidly at large distances. The resultant underbinding is largely corrected by the AC-LDA potential whose orbital energies correlate well with OEP orbital energies, with typical differences on the order of 0.5 eV. However larger differences between AC-LDA and OEP orbital energies are also observed, particularly for unoccupied orbitals and the reason for this is discussed. As an illustration of how the OEP might be used in practical calculations, we give an example from time-dependent DFT where use of the OEP instead of the AC-LDA potential leads to significant improvement in a key #sigma#->#pi#~* excitation energy of ethylene.
机译:优化的有效电势(OEP)是(在一定的线性响应近似范围内)密度泛函理论(DFT)的精确交换相关电势。在DEMON-DYNARHO程序中,我们已在仅交换级别实现了OEP,而没有使用识别分辨率技术对四中心积分进行评估。我们指出,在使用有限基集方法处理OEP的渐近行为时必须格外小心。我们的结果与以前使用类似OEP电位的工作进行了比较。我们的OEP轨道能量与实验电离势进行了比较。 Hartree-Fock(HF)轨道能量,以及具有和不具有渐近校正(AC)的局部密度近似(LDA)势能的轨道能量。我们发现OEP轨道能量比HF轨道能量更好地近似于实验电离势。除了分子依赖性的刚性位移外,LDA轨道能量还与OEP轨道能量密切相关,这是由于众所周知的事实,即LDA电位在很远的距离上下降得太快。由此产生的欠约束力很大程度上由AC-LDA电位校正,该电位的轨道能量与OEP轨道能量高度相关,典型差异约为0.5 eV。但是,还观察到了AC-LDA和OEP轨道能量之间的较大差异,特别是对于未占用的轨道,并讨论了其原因。为了说明在实际计算中如何使用OEP,我们从与时间有关的DFT中给出一个示例,在该示例中,使用OEP代替AC-LDA电位可显着改善关键的#sigma#->#pi#乙烯的激发能。

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