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Phys 498CQM Lecture 6

Wed. March 7, 2001
Lecturer: Richard Martin
HW2
Reading:
Thijssen, Ch 4, p 45 - 57.
(Also Koonin p. 72 - 84)

Outline

The Many-Body Hamiltonian for Electrons and Hartree-Fock Theory
  1. The many-body electron problem
    • General theoretical forms
      • The general many-body hamiltonian for electrons and nuclei
      • The many-body antisymmetric wavefunction
      • Energy as a functional of the wavefunction
      • Variational principle for the ground state
  2. General theory of functionals F[f(x)]
    • Functional derivatives
  3. Hartree-Fock uncorrelated approximate wavefunction
    • General Slater determinant spin-orbital form
      (Why a "Slater Determinant" instead of a "dirac Determinant"?)
    • Energy = sum of single body terms, direct coulomb, and exchange
    • Solution by minimization using variational theorem and Lagrange multipliers for orthonormality constraints
    • Nonlinear "Schroedinger-like" Equations, with difficult non-local exchange terms
    • Two-electron example (following Koonin, also similar to Thijssen)
    • Restricted Hartree Fock approximations: Open Shell vs. Closed Shell
      • "Spin Restricted": Occupy states just as in a non-interacting theory
        Require equal spin up and spin down orbitals
        Correct solution for cases which are "closed shell"
      • "Orbital Restricted": Allow unequal determinants and orbitals for up and down spins
        Require potential for each state (n,l,ml,ms) to depend only on (n,l,ms); i.e., independent of ml
        Essential for some cases - like H atom!
        Approximate solution for "Open Shell systems"
      • "Unrestricted": no assumptions on symmetry of potential
  4. Numerical methods for solution of equations for an atom
    • Of of the few cases where the H-F equations can be solved directly by integrating differential equations
    • Continuation of discussion of solution of eigenvalue problems related to Homework 2
    • Hartree-Fock solution for atom requires solution of coupled Schroedinger-like and Poisson Eqs.
    • Explicit formulas take advantage of expansions for Coulomb terms
    • Equations for full Unrestricted case prepared by Tim Wilkens based upon formulas from Slater and other sources
    • Ouline for computer program for solution. More later

Last Modified Feb. 7
Email question/comments/corrections to rmartin@uiuc.edu .