For harmonic-oscillator lowering and raising operators $\hat a,\hat a^\dagger$, the energy eigenstate $|n\rangle$ is also an eigenstate of $(\hat a^\dagger)^2\hat a^2$. Its eigenvalue is
Apply the two lowering operators first: $\hat a^2|n\rangle=\sqrt{n(n-1)}|n-2\rangle$. The two raising operators return the state with another factor $\sqrt{n(n-1)}$. Their product gives $(\hat a^\dagger)^2\hat a^2|n\rangle=n(n-1)|n\rangle$, A. This also gives zero for n = 0 or 1.
More One dimensional potentials: step potential, finite rectangular well, tunnelling from a potential barrier, particle in 1,2,3-dimensional box, particle in single and double delta function potentials, 1,2,3 dimensional harmonic oscillator: concept of degeneracy questions
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