The hartree-fock method for many-electron problems

點閱:9

作者:S.M. Shiau

出版年:c2017

出版社:Tamkang University Press

出版地:New Taipei City

集叢名:專業叢書:PS015

格式:PDF,JPG

ISBN:978-986-5608-48-4 ; 986-5608-48-0


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借閱說明

Back ground of the Hartree-Fock method
 
Introduction
 
The physical systems, such as atoms, molecules and solids, consist not only of electrons but also of nuclei, and each of these particles moves in the field generated by the others.
 
The Hartree-Fock (HF) approach is to consider the nuclei as being fixed, and to solve the Schrodinger equation for the electronic system in the field of the static nuclei.
 
This approach is called the Born-oppenheimer approximation. It remains then to solve for the electronic structure.
 
The wave functions of the many-electron system have the form of an anti-symmetries product of one-electron wave functions.
 
This restriction leads to an effective Schrodinger equation for the individual one-electron wave functions (call orbitals) with a potential determined by the orbitals occupied by the other electrons.
 
The solution to the effective Schrodinger equation must be found iteratively in a self-consistency procedure.
 
In the variational approach, correlations between the electrons are neglected to some extent.
 
In particular, the coulomb repulsion between the electrons is represented in an averaged way.
 
In the HF approach, the effective interaction caused by the fact that the electrons are fermions, obeying Pauli's principle, and want to keep apart if they have the same spin, is included.
 
HF approximation (neglect the coulomb correlations) is improved by constructing a many-electron state as linear combination of Slater determinants.
 
These determinants are constructed from the ground state by excitation: the first determinant is the Hartree-Fock ground state and the second one is the first excited state (within the spectrum determined selfconsistently for the ground state) and so on.
 
The matrix elements of the Hamiltonian between these Slater determinants are calculated and the resulting Hamilton matrix (which has a dimension equal to the number of Slater determinants taken into account) is diagonalized.
 
The resulting state is then a linear combination of Slater determinants.

  • References(p.220)