This is a common exercise in the classroom. They always check the cases when $E>0$ and $V<E<0$ for a finite negative well $V<0$.
But what about the case $E<V$. What happens here?
This is a common exercise in the classroom. They always check the cases when $E>0$ and $V<E<0$ for a finite negative well $V<0$.
But what about the case $E<V$. What happens here?
For any state $|\psi\rangle$ we have that $$ \langle H \rangle = \frac{1}{2m}\langle p^2\rangle + \langle V \rangle\;. $$
As it is a square $\langle p^2 \rangle \ge 0$.
Now if we have that, for all $x$, $V(x) \ge V_{min}$, we can say $$ \langle V \rangle = \int dx\; \psi^*(x) V(x) \psi(x) \ge V_{min} \int dx |\psi(x)|^2 = V_{min}\;. $$ Putting this together we have that $$ \langle H \rangle \ge 0 + V_{min}\;. $$ Since all states have an energy expectation greater than or equal to $V_{min}$, there can be no eigenstates of $H$ with energy less than $V_{min}$