Multiresolution quantum chemistry in multiwavelet bases: excited states from time-dependent Hartree-Fock and density functional theory via linear response

被引:27
作者
Yanai, Takeshi [1 ]
Fann, George I. [2 ]
Beylkin, Gregory [3 ]
Harrison, Robert J. [4 ,5 ]
机构
[1] Inst Mol Sci, Dept Theoret & Computat Mol Sci, Okazaki, Aichi 4448585, Japan
[2] Oak Ridge Natl Lab, Div Math & Comp Sci, Oak Ridge, TN 37831 USA
[3] Univ Colorado, Dept Appl Math, Boulder, CO 80309 USA
[4] SUNY Stony Brook, Inst Adv Computat Sci, Stony Brook, NY 11794 USA
[5] Brookhaven Natl Lab, Computat Sci Ctr, Upton, NY 11973 USA
基金
美国国家科学基金会;
关键词
EXCITATION-ENERGIES; LOCAL-DENSITY; BASIS-SETS; APPROXIMATION; ALGORITHMS;
D O I
10.1039/c4cp05821f
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
A fully numerical method for the time-dependent Hartree-Fock and density functional theory (TD-HF/DFT) with the Tamm-Dancoff (TD) approximation is presented in a multiresolution analysis (MRA) approach. From a reformulation with effective use of the density matrix operator, we obtain a general form of the HF/DFT linear response equation in the first quantization formalism. It can be readily rewritten as an integral equation with the bound-state Helmholtz (BSH) kernel for the Green's function. The MRA implementation of the resultant equation permits excited state calculations without virtual orbitals. The integral equation is efficiently and adaptively solved using a numerical multiresolution solver with multiwavelet bases. Our implementation of the TD-HF/DFT methods is applied for calculating the excitation energies of H-2, Be, N-2, H2O, and C2H4 molecules. The numerical errors of the calculated excitation energies converge in proportion to the residuals of the equation in the molecular orbitals and response functions. The energies of the excited states at a variety of length scales ranging from short-range valence excitations to longrange Rydberg-type ones are consistently accurate. It is shown that the multiresolution calculations yield the correct exponential asymptotic tails for the response functions, whereas those computed with Gaussian basis functions are too diffuse or decay too rapidly. We introduce a simple asymptotic correction to the local spin-density approximation (LSDA) so that in the TDDFT calculations, the excited states are correctly bound.
引用
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页码:31405 / 31416
页数:12
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