For a test wavefunction ,
Thus the canonical commutation relation is
The time-dependent Schrödinger equation is
Differentiating and using the Schrödinger equation and its adjoint gives the Ehrenfest theorem
Using and ,
With , the canonical commutators give
It follows that
Therefore rotational symmetry of the isotropic oscillator gives
In polar coordinates, and
Consequently
The two states are orthogonal. They are degenerate energy eigenstates, so their coefficients acquire the same overall time-dependent phase; equivalently, makes constant. For the normalized state
the angular momentum of a complex-coordinate Gaussian state is therefore

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