Principles of Quantum Mechanics · Problem 12.5.12

Rotational Invariance and Angular Momentum — R. Shankar

Physics — Quantum Mechanics · parity-spherical-harmonics

Problem

Since L2L^2 and LzL_z commute with Π\Pi, they should share a basis with YlmY_l^m. Verify that YlmΠ(−1)lYlmY_l^m \Pi (-1)^l Y_l^m. (First show that θ→π−θ\theta \to \pi - \theta, ϕ→ϕ+π\phi \to \phi + \pi under parity. Prove the result for YllY_l^l. Verify that L−L_- does not alter the parity, thereby proving the result for all YlmY_l^m.)

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