From and the commutator product rule,Consequently, if ,Thus the creation operator raises the energy eigenvalue by , and the annihilation operator lowers it by , provided the resulting vector is nonzero. The zero vector is not an eigenstate; in particular the ground state will be annihilated by . The displayed operator identity holds even in that case.
The squared norm is obtained by moving the adjoint operator to the other side of the inner product:For an energy eigenstate, this isSince a squared norm is nonnegative, every nonzero energy eigenstate has . Moreover exactly when .
Write . Repeated application of the annihilation operator lowers the energy eigenvalue in steps of . The lower bound from part (ii) forces this process to stop. To see why it also quantizes the starting energy, writeThe first lowering steps have positive squared norms. If , the next step is also nonzero by part (ii), and its energy would be , contradicting the bound. Thus , andExistence of the ground state can also be checked directly in the position representation. The equation iswhose solution is proportional to . This Gaussian function is square-integrable, so it gives an actual ground state. Its normalization can be chosen using the Gaussian integral.
All the displayed levels occur: for a nonzero state at ,Thus repeated raising creates a nonzero energy eigenstate at every .
Let have energy and put . The lowering norm formula gives, inductively,In particular is a nonzero ground state. By the assumed nondegeneracy, it equals for some .
It remains to show that raising this vector recovers , rather than merely another state at the same energy. On an energy eigenstate at , factorization gives . Iterating the factorization down the ladder yieldsApplying to therefore provesFor this is the original ground-state assumption. This proves nondegeneracy propagated by an oscillator ladder: every energy eigenspace is one-dimensional if the ground state is nondegenerate.
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