The Pauli Exclusion Principle — Question 9

Section 40-6 · Physics pages 6688–6689

Question 9 The exchange term changes two-electron interaction energies For two orthonormal spatial orbitals u,v define normalized symmetric and antisymmetric states ψ± = [u(1)v(2) ± v(1)u(2)]/ √ 2. A spin-independent symmetric interaction V has direct integral J and real exchange integral K: J = ⟨uv|V |uv⟩= ⟨vu|V |vu⟩, K = ⟨uv|V |vu⟩. triplet: J −K singlet: J + K ∆E Schematic; labels, not drawing lengths, specify the data. (a) Derive each interaction expectation. (b) For K > 0, compare singlet and triplet energies when their one-electron energies are equal.
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Question 9 - Solution The exchange term changes two-electron interaction energies triplet: J −K singlet: J + K ∆E (a) Method and calculation ⟨V ⟩± = 1 2[J + J ± K ± K]. ⟨V ⟩+ = J + K, ⟨V ⟩−= J −K . (b) Interpretation and further calculation Singlet: symmetric space; triplet: antisymmetric space. Es −Et = (J + K) −(J −K) = 2K > 0 . Physical check The energy ordering here follows the supplied interaction integrals, not exclusion alone. Different orbital occupancies add one-electron energy costs that must also be considered.

Question 9

The exchange term changes two-electron interaction energies

For two orthonormal spatial orbitals u,v define normalized symmetric and antisymmetric states ψ±=[u(1)v(2)±v(1)u(2)]/2\psi_\pm=[u(1)v(2)\pm v(1)u(2)]/\sqrt2. A spin-independent symmetric interaction V has direct integral J and real exchange integral K: J=⟨uv|V|uv⟩=⟨vu|V|vu⟩J=\langle uv|V|uv\rangle=\langle vu|V|vu\rangle, K=⟨uv|V|vu⟩K=\langle uv|V|vu\rangle.

Diagram shown in the original SVG worksheet.

  1. Derive each interaction expectation.

  2. For K>0K>0, compare singlet and triplet energies when their one-electron energies are equal.

Question 9 - Solution

The exchange term changes two-electron interaction energies

Diagram shown in the original SVG worksheet.

(a) Method and calculation

⟨V⟩±=12[J+J±K±K].\langle V\rangle_\pm=\tfrac12[J+J\pm K\pm K].⟨V⟩+=J+K,⟨V⟩−=J−K.\boxed{\langle V\rangle_+=J+K,\quad\langle V\rangle_-=J-K}.

(b) Interpretation and further calculation

Singlet: symmetric space;triplet: antisymmetric space.\text{Singlet: symmetric space};\qquad\text{triplet: antisymmetric space}.Es−Et=(J+K)−(J−K)=2K>0.\boxed{E_s-E_t=(J+K)-(J-K)=2K>0}.

Physical check

The energy ordering here follows the supplied interaction integrals, not exclusion alone. Different orbital occupancies add one-electron energy costs that must also be considered.