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Phys 498CQM Lecture # 7
Monday, February 12, 2001
Lecturer: Richard Martin
Reading:
Thijssen Ch. 4
See also:Koonin p. 72 - 84
Outline: Hartree-Fock Theory for Atoms
Continue discussion of solving 1-d Schr. Eq. by "shooting" method
Continue discussion of derivation of Hartree-Fock equations
Equations in the 2-electron case
Equations in the many-electron case
Meaning of eigenvalues - Koopman's theorem
Gap for adding vs subtracting particles
Solution of Restricted Hartree-Fock equations for spherical atoms
Closed shells, and with one more or one less electron, are spherical
Restricted HF (equal orbitals for up and down spin) apppropriate only for cases with paired spins (Closed Shell systems)
Regular or log grids?
Numerical solution of radial equations
For other cases, one can let the spin be unrestricted but still make the spherical approximation for the spacial potential (Spin unrestricted)
Full unrestricted case
Expressions for exchange and Hartree potentials in general case
Consequences
Self-Consistency in potential and wavefunctions
Starting guess - hydrogenic orbitals
Programs written by T. J. Wilkens
Examples of solutions: H, He, Li, Be, B, Ne.
Last Modified Feb. 11 Email question/comments/corrections to
rmartin@uiuc.edu
.