Introduction to Quantum Mechanics · Problem 6.17

Symmetries and Conservation Laws — David J. Griffiths

Physics — Quantum Mechanics · rotation_angular_momentum

Problem

Consider the action of an infinitesimal rotation about the n\mathbf{n} axis of an angular momentum eigenstate ψnℓm\psi_{n\ell m}. Show that R^n(δ) ψnℓm=∑m′Dm′m ψn ℓ m′,\hat{R}_{\mathbf{n}}(\delta)\,\psi_{n\ell m} = \sum_{m'} D_{m'm}\,\psi_{n\,\ell\,m'}, and find the complex numbers Dm′mD_{m'm} (they will depend on δ\delta, n\mathbf{n}, and ℓ\ell as well as mm and m′m'). This result makes sense: a rotation doesn't change the magnitude of the angular momentum (specified by ℓ\ell) but does change its projection along the zz axis (specified by mm).

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