Assume a standard one-particle, non-relativistic Hamiltonian of the form \begin{equation} H=\frac{p^2}{2m}+V(r) \end{equation} and denote its eigenvalues as $E_{n,\tau}$, where $n$ is the principal quantum number and $\tau$ represents all the other quantum numbers, if any.
Is it possible to derive a lower bound on $E_{n+1,\tau}-E_{n,\tau}$, i.e. on the energy gap between consecutive levels with the same quantum numbers? My intuition is that long-range potentials should allow smaller gaps (cf. the Coulomb potential, where the gap gets infinitely small as $n\to\infty$), but I haven't managed to express this quantitatively.