Principles of Quantum Mechanics · Problem 12.5.9

Rotational Invariance and Angular Momentum — R. Shankar

Physics — Quantum Mechanics · angular-momentum-hermiticity

Problem

Show that L2L^2 above is Hermitian in the sense ∫ψ1∗(L2ψ2) dΩ=[∫ψ2∗(L2ψ1) dΩ]∗\int \psi_1^*(L^2\psi_2)\, d\Omega = \left[\int \psi_2^*(L^2\psi_1)\, d\Omega\right]^*

Related theory

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