The Hamiltonian operator separates into two commuting one-dimensional quantum harmonic oscillators. Write
Products of harmonic oscillator eigenfunctions give
Here is the physicists' Hermite polynomial, so , and . The first six energy eigenstates, ordered with multiplicity, are
For this two-dimensional oscillator level ordering, the excitation energies obey
Every state with costs at least , so none has been missed. Equalities within the list occur when . Then the two-dimensional isotropic harmonic oscillator has
The quantum degeneracy counts with . The six listed states occupy three distinct energy levels, of quantum degeneracies one, two and three.

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