Dear Class,
Could you do 4.23 for Wednesday?
I'm sorry that the discussion of the angular-momentum operators in position space wasn't clearer. But it should make sense that the spherical harmonics are eigenfunctions of L2 and L_z. The exp(i m phi) factor automatically makes them eigenfunctions of L_z,. I hope the argument about writing the Hamiltoian in terms of a radial part and L2/2mr2 makes it clear why R(r)Y_l^m(\theta,\phi) is an eigenfunction of L2. If not, let me know.
Signed,
Your Prof

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