The Pauli Exclusion Principle — Question 5

Section 40-6 · Physics pages 6680–6681

Question 5 Parallel spins require an antisymmetric spatial wave function Two electrons have the symmetric spin state | ↑↑⟩and occupy distinct orthonormal spatial orbitals u and v. Neglect interactions. x1 x2 node: x1 = x2 Schematic; labels, not drawing lengths, specify the data. (a) Construct their normalized spatial state. (b) Evaluate its amplitude at equal positions and explain the resulting same-spin coincidence suppression.
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Question 5 - Solution Parallel spins require an antisymmetric spatial wave function x1 x2 node: x1 = x2 (a) Method and calculation Ψspace(1, 2) = C[u(1)v(2) −v(1)u(2)]. Ψspace = u(1)v(2) −v(1)u(2) √ 2 . (b) Interpretation and further calculation Ψspace(r, r) = u(r)v(r) −v(r)u(r) √ 2 = 0. |Ψspace(r, r)|2 = 0 . Physical check This zero follows from exchange antisymmetry even with no repulsive force. Opposite-spin electrons are not subject to the same spatial coincidence zero.

Question 5

Parallel spins require an antisymmetric spatial wave function

Two electrons have the symmetric spin state |↑↑⟩|\uparrow\uparrow\rangle and occupy distinct orthonormal spatial orbitals u and v. Neglect interactions.

Diagram shown in the original SVG worksheet.

  1. Construct their normalized spatial state.

  2. Evaluate its amplitude at equal positions and explain the resulting same-spin coincidence suppression.

Question 5 - Solution

Parallel spins require an antisymmetric spatial wave function

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ψspace(1,2)=C[u(1)v(2)−v(1)u(2)].\Psi_{\mathrm{space}}(1,2)=C[u(1)v(2)-v(1)u(2)].Ψspace=u(1)v(2)−v(1)u(2)2.\boxed{\Psi_{\mathrm{space}}=\frac{u(1)v(2)-v(1)u(2)}{\sqrt2}}.

(b) Interpretation and further calculation

Ψspace(𝒓,𝒓)=u(𝒓)v(𝒓)−v(𝒓)u(𝒓)2=0.\Psi_{\mathrm{space}}(\boldsymbol r,\boldsymbol r)=\frac{u(\boldsymbol r)v(\boldsymbol r)-v(\boldsymbol r)u(\boldsymbol r)}{\sqrt2}=0.|Ψspace(𝒓,𝒓)|2=0.\boxed{|\Psi_{\mathrm{space}}(\boldsymbol r,\boldsymbol r)|^2=0}.

Physical check

This zero follows from exchange antisymmetry even with no repulsive force. Opposite-spin electrons are not subject to the same spatial coincidence zero.