The orbital angular momentum operator is
Using and ,
and
Thus the rotation commutators for orbital angular momentum are
Contract the two Levi-Civita symbols:
Moving momenta past positions with
gives the squared orbital angular momentum in position and momentum operators:
Therefore
In position representation,
and
Also . Substitution into the Cartesian identity gives
because every radial derivative cancels. Hence
the spherical Laplacian from orbital angular momentum.
The first excited hydrogen eigenspace is the four-dimensional space
The first vector is the state and the other three are the states. All have the same unperturbed energy .
The states diagonalize :
The perturbation therefore introduces no mixing. The orbital-angular-momentum-squared perturbation of hydrogen leaves
at energy
while
remain triply degenerate at
These statements are exact because the unperturbed Hamiltonian commutes with .
Part (a) gives
Hence both operators preserve the magnetic quantum number . They are also odd under parity, while has parity . Their matrix elements between states of equal parity vanish. The position-momentum selection rules in the first excited hydrogen eigenspace therefore leave only the coupling between
The states decouple, and all diagonal matrix elements vanish.
In the ordered basis , remove the common energy and write
Let
The rotating-frame amplitudes obey a constant Schrödinger equation
Put
Since ,
For the initial amplitudes , the exact coefficients are therefore
and
Restoring the common unperturbed phase, the solution is
This is the rotating-frame solution for a harmonically driven two-level system.

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