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I'm pretty sure this is correct, but could someone verify for rigor?
Problem
Two observables A_1 and A_2, which do not involve time explicitly, are known not to commute, yet we also know that A_1 and A_2 both commute with the Hamiltonian. Prove that the energy eigenstates are, in general, degenerate. Are there exceptions?
The attempt at a solution
Since [H,A_1]=0, we know that there are complete eigenkets that A_1 and H share. The same is true for A_2. Now, generally, two observables that do not commute do not share eigenkets. Thus, we know that there exist two distinct eigenstates such that H|a\ket = e|a\ket; particularly, each |a\ket can be brought from the eigenkets of A_1,A_2.
Problem
Two observables A_1 and A_2, which do not involve time explicitly, are known not to commute, yet we also know that A_1 and A_2 both commute with the Hamiltonian. Prove that the energy eigenstates are, in general, degenerate. Are there exceptions?
The attempt at a solution
Since [H,A_1]=0, we know that there are complete eigenkets that A_1 and H share. The same is true for A_2. Now, generally, two observables that do not commute do not share eigenkets. Thus, we know that there exist two distinct eigenstates such that H|a\ket = e|a\ket; particularly, each |a\ket can be brought from the eigenkets of A_1,A_2.