The Pauli Exclusion Principle — Question 3

Section 40-6 · Physics pages 6676–6677

Question 3 Nonorthogonal orbitals change the normalization of an antisymmetric pair Two normalized spin orbitals a and b have real overlap S = ⟨a|b⟩= 3/5. Use Ψ = C[a(1)b(2) −b(1)a(2)] with C positive. a b S Schematic; labels, not drawing lengths, specify the data. (a) Find the normalization constant. (b) Discuss the limit S →1 and why the formula cannot normalize two identical orbitals.
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Question 3 - Solution Nonorthogonal orbitals change the normalization of an antisymmetric pair a b S (a) Method and calculation ∥Ψ∥2 = 2C2(1 −|S|2). C = [2(1 −9/25)]−1/2 = 5/(4 √ 2) . (b) Interpretation and further calculation S →1 : ∥a(1)b(2) −b(1)a(2)∥2 →0. b = a : Ψ ≡0 ⇒no normalized duplicate state . Physical check A diverging normalization factor at coincident orbitals does not rescue the exactly zero determinant. Distinct limiting paths may approach different second orbitals after orthogonalization.

Question 3

Nonorthogonal orbitals change the normalization of an antisymmetric pair

Two normalized spin orbitals a and b have real overlap S=⟨a|b⟩=3/5S=\langle a|b\rangle=3/5. Use Ψ=C[a(1)b(2)−b(1)a(2)]\Psi=C[a(1)b(2)-b(1)a(2)] with C positive.

Diagram shown in the original SVG worksheet.

  1. Find the normalization constant.

  2. Discuss the limit S→1S\to1 and why the formula cannot normalize two identical orbitals.

Question 3 - Solution

Nonorthogonal orbitals change the normalization of an antisymmetric pair

Diagram shown in the original SVG worksheet.

(a) Method and calculation

∥Ψ∥2=2C2(1−|S|2).\|\Psi\|^2=2C^2(1-|S|^2).C=[2(1−9/25)]−1/2=5/(42).\boxed{C=[2(1-9/25)]^{-1/2}=5/(4\sqrt2)}.

(b) Interpretation and further calculation

S→1:∥a(1)b(2)−b(1)a(2)∥2→0.S\to1:\quad\|a(1)b(2)-b(1)a(2)\|^2\to0.b=a:Ψ≡0⇒no normalized duplicate state.b=a:\quad\Psi\equiv0\Rightarrow\boxed{\text{no normalized duplicate state}}.

Physical check

A diverging normalization factor at coincident orbitals does not rescue the exactly zero determinant. Distinct limiting paths may approach different second orbitals after orthogonalization.