Someone studying the exchange hole in a Slater determinant argues:"Hartree-Fock…

PHYSICS · Multi-part · Fermi University Physics · Quantum Mechanics · Atomic, Molecular & Optical Physics · Many-electron atoms and the periodic table

Deriving the Spectrum, Ch Self-consistent fields and correlation

Problem

Someone studying the exchange hole in a Slater determinant argues:"Hartree-Fock exchange makes each electron dig a hole in the density of the other electrons, and this hole lowers the energy. The two electrons of H−\mathrm{H}^- (one spin ↑\uparrow, one spin ↓\downarrow) are both present in the Hartree-Fock determinant, so each should dig a hole around the other, exactly as the same-spin electrons do in helium's triplet state. Hartree-Fock's energy for H−\mathrm{H}^-, −0.4879 Eh-0.4879\,E_{\rm h}, should therefore already include as much mutual avoidance between the two electrons as is physically possible. The fact that this lies above the −0.5 Eh-0.5\,E_{\rm h} needed for binding (the energy of a free H atom plus a free electron at rest) must be some other failure of the method, not a missing hole." ((a)) Identify the error in this reasoning. ((b)) State which pairs of electrons in a Slater determinant actually carry an exchange hole, and why. ((c)) Explain what physically distinguishes the avoidance between H−\mathrm{H}^-'s two electrons that Hartree-Fock does include from the avoidance that is missing.

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