If an operator commutes with the Hamiltonian of a problem, must it always admit degeneracy? It appears that not necessarily. For example, the parity operator commutes with the Hamiltonian of a free particle as well as that of the 1-D linear harmonic oscillator. But in the former case, we have two-fold degeneracy for a given energy and no degeneracy for the latter. Does it mean that [P,H]=0 is not the sufficient condition to have degeneracy in the energy eigenstates?
Answer
If an operator commutes with the Hamiltonian of a problem, must it always admit degeneracy?
No. The identity always commutes with the Hamiltonian, yet we don't generally find all energy levels to be degenerate.
Does it mean that [P,H]=0 is not the sufficient condition to have degeneracy in the energy eigenstates?
Yes. It is not a sufficient condition.
Let A,B be any two self-adjoint operators that commute, [A,B]=0. Define the eigenvectors of A through
A|a⟩=a |a⟩
Now we prove that B|a⟩ is also an eigenvector of A: A(B|a⟩)=BA|a⟩=a(B|a⟩)
Welp, that was easy.
We could naively say that a is degenerate, because both |a⟩ and B|a⟩ have the same eigenvalue, but this breaks down if |a⟩ is an eigenvector of B, because in that case B|a⟩∝|a⟩ and there is no degeneracy!
Therefore, if |a⟩ is not an eigenvector of B we find that a is degenerate, with at least two eigenvectors, |a⟩ and B|a⟩. If |a⟩ is an eigenvector of B we can't conclude anything about the degeneracy of a.
In the case B=I, we obviously have [H,B]=0, but as any vector is an eigenvector of I, the fact that these operators commute gives no information about energy-degeneracies.
In the case of a free particle, the parity operators acts on kets by changing the sign, P|\boldsymbol p\rangle=|-\boldsymbol p\rangle, which is not proportional to |\boldsymbol p\rangle (a.e.), and therefore we do have the two-fold degeneracy you said.
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