A Modern Approach to Quantum Mechanics · Problem 9.6

Translational and Rotational Symmetry in the Two-Body Problem — John S. Townsend

Physics — Quantum Mechanics · vector-operator-rotation-commutation

Problem

Show that the commutation relations of the orbital angular momentum operators can be cast in a similar form as for r^\hat{\mathbf{r}} and p^\hat{\mathbf{p}} under rotations: [L^z,L^x]=iℏL^y[L^z,L^y]=−iℏL^x[L^z,L^z]=0[\hat{L}_z, \hat{L}_x] = i\hbar \hat{L}_y \qquad [\hat{L}_z, \hat{L}_y] = -i\hbar \hat{L}_x \qquad [\hat{L}_z, \hat{L}_z] = 0 All vector operators must behave the same way when they are rotated.

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