Communication: Kohn-Sham theory for excited states of Coulomb systems

被引:40
作者
Ayers, P. W. [1 ]
Levy, M. [2 ,3 ,4 ]
Nagy, A. [5 ]
机构
[1] McMaster Univ, Dept Chem & Chem Biol, Hamilton, ON L8S 4M1, Canada
[2] N Carolina Agr & Tech State Univ, Dept Phys, Greensboro, NC 27411 USA
[3] Duke Univ, Dept Chem, Durham, NC 27708 USA
[4] Tulane Univ, Dept Chem, New Orleans, LA 70118 USA
[5] Univ Debrecen, Dept Theoret Phys, H-4010 Debrecen, Hungary
基金
加拿大自然科学与工程研究理事会;
关键词
DENSITY-FUNCTIONAL THEORY; LONG-RANGE BEHAVIOR; FRACTIONALLY OCCUPIED STATES; ATOMIC ELECTRON-DENSITY; EXCITATION-ENERGIES; ASYMPTOTIC-BEHAVIOR; NATURAL ORBITALS; CUSP CONDITIONS; CHARGE-DENSITY; EXCHANGE;
D O I
10.1063/1.4934963
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
For obtaining individual excited-state energies and densities of Coulomb electronic systems, by means of an energy stationary principle, it was shown previously that there exists a universal functional of the density, F-Coul[rho], for the kinetic plus electron-electron repulsion part of the total energy. Here, we make knowledge of the existence of F-Coul[rho] practical for calculation by identifying T-s(Coul)[rho], the non-interacting kinetic energy component of F-Coul[rho], and by showing that T-s(Coul)[rho] may be computed exactly by means of orbitals that are obtained through a set of single-particle Kohn-Sham equations. Constraints for obtaining accurate approximations to the remaining unknown component of F-Coul[rho] are presented. (C) 2015 AIP Publishing LLC.
引用
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页数:4
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