The orbital angular momentum operator isUsing and ,andThus 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
gives the squared orbital angular momentum in position and momentum operators:Therefore
In position representation,andAlso . Substitution into the Cartesian identity givesbecause every radial derivative cancels. Hencethe spherical Laplacian from orbital angular momentum.
The first excited hydrogen eigenspace is the four-dimensional spaceThe 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 leavesat energywhileremain triply degenerate atThese statements are exact because the unperturbed Hamiltonian commutes with .
Part (a) givesHence 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 betweenThe states decouple, and all diagonal matrix elements vanish.
In the ordered basis , remove the common energy and writeLetThe rotating-frame amplitudes obey a constant Schrödinger equationPutSince ,For the initial amplitudes , the exact coefficients are thereforeandRestoring the common unperturbed phase, the solution isThis is the rotating-frame solution for a harmonically driven two-level system.
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