Energy surface, chemical potentials, Kohn-Sham energies in spin-polarized density functional theory

被引:16
|
作者
Gal, T. [1 ]
Geerlings, P. [1 ]
机构
[1] Free Univ Brussels VUB, Dept Gen Chem ALGC, B-1050 Brussels, Belgium
来源
JOURNAL OF CHEMICAL PHYSICS | 2010年 / 133卷 / 14期
关键词
EXCHANGE-CORRELATION POTENTIALS; ORBITAL ENERGIES; DERIVATIVE DISCONTINUITIES; EXCITATION-ENERGIES; ELECTRON-DENSITIES; KOOPMANS THEOREM; ENSEMBLES; NUMBER; ANALOG; EIGENVALUES;
D O I
10.1063/1.3467898
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
On the basis of the zero-temperature grand canonical ensemble generalization of the energy E[N, N-s, upsilon, B] for fractional particle N and spin N-s numbers, the energy surface over the (N, N-s) plane is displayed and analyzed in the case of homogeneous external magnetic fields B((r) over bar). The (negative of the) left-/right-side derivatives of the energy with respect to N, N-up arrow, and N-down arrow give the fixed-N-s, spin-up, and spin-down ionization potentials/electron affinities, respectively, while the derivative of E[N, N-s, upsilon, B] with respect to N-s gives the (signed) half excitation energy to the lowest-lying state with N-s increased (or decreased) by 2. The highest occupied and lowest unoccupied Kohn-Sham spin-orbital energies are identified as the corresponding spin-up and spin-down ionization potentials and electron affinities. The excitation energies to the lowest-lying states with N-s + 2 can be obtained as the differences between the lowest unoccupied and the opposite-spin highest occupied spin-orbital energies, if the (N, N-s) representation of the Kohn-Sham spin-potentials is used. The cases where the convexity condition on the energy does not hold are also discussed. Finally, the discontinuities of the energy derivatives and the Kohn-Sham potential are analyzed and related. (C) 2010 American Institute of Physics. [doi:10.1063/1.3467898]
引用
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页数:16
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