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For the three-dimensional isotropic harmonic oscillator, substituting $X_i=\sqrt{\hslash /(2\mu \omega )}(A_i+A_i^{†})$ and $P_i=i\sqrt{\mu \hslash \omega /2}(A_i^{†}-A_i)$ into $L_i={\epsilon }_{ijk}{X}_j{P}_k$ gives $L_i=-i\hslash {\epsilon }_{ijk}{A}_j^{†}{A}_k$. On the first-excited Cartesian states $|j⟩=A_j^{†}|0⟩$, this is the three-dimensional vector representation and $L^2|j⟩=2{\hslash }^2|j⟩$, so the whole first-excited level has orbital quantum number $\ell =1$.

The Hamiltonian is the sum of three commuting one-dimensional harmonic-oscillator Hamiltonians. Its product eigenstates arewith energiesEquivalently, the level with $N=n_x+n_y+n_z$ has energy $E_N=\hslash \omega (N+3/2)$, as in the three-dimensional isotropic harmonic oscillator.

Up to normalization, the ground-state wavefunction isIt is radial, so $\nabla {\Psi }_{000}$ is parallel to the position vector. Since the orbital angular momentum is $L=-i\hslash r\times \nabla$, every component of $L$ annihilates this state. Thereforeand the ground state has $\ell =m=0$.

The first excited level has $N=1$ and is spanned byThe statesatisfies $L_z{\Phi }_0=0$. Applying the ladder operators givesHence convenient $m=\pm 1$ eigenstates areup to normalization and irrelevant overall phases.

Finally, the isotropic Hamiltonian is rotationally invariant. The rotational invariance of a central-potential Hamiltonian givesThese commuting self-adjoint operators can be simultaneously diagonalized within each energy eigenspace, which is why joint eigenstates of $H,L^2,L_z$ must exist.