Consider the three angular momentum variables in classical mechanics:
lx=ypz−zpyly=zpx−xpzlz=xpy−ypx
(1) Construct Lx, Ly, and Lz, the quantum counterparts, and note that there are no ordering ambiguities.
(2) Verify that {lx,ly}=lz [see Eq. (2.7.3) for the definition of the PB].
(3) Verify that [Lx,Ly]=iℏLz.