Introduction to Quantum Mechanics · Problem 7.25

Time-Independent Perturbation Theory — David J. Griffiths

Physics — Quantum Mechanics · wigner_eckart_theorem

Problem

Use the Wigner–Eckart theorem (Equations 6.59–6.61) to prove that the matrix elements of any two vector operators, V\mathbf{V} and W\mathbf{W}, are proportional in a basis of angular-momentum eigenstates: ⟨n ℓ′ m′∣V∣n ℓ m⟩=α⟨n ℓ′ m′∣W∣n ℓ m⟩.\langle n\,\ell'\,m' | \mathbf{V} | n\,\ell\,m \rangle = \alpha \langle n\,\ell'\,m' | \mathbf{W} | n\,\ell\,m \rangle. Comment: With ℓ\ell replaced by jj (the theorem holds regardless of whether the states are eigenstates of orbital, spin, or total angular momentum), V=L+2S\mathbf{V} = \mathbf{L} + 2\mathbf{S} and W=J\mathbf{W} = \mathbf{J}, this proves Equation 7.77.

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