I) It seems that the question(v1) is essentially asking the following:
If a 1D potential $V$ is a non-negative function on the real line $\mathbb{R}$, except for a compact interval $[a,b]$ where it is allowed to be negative, then would the number of (bounded) negative energy eigenstates for the corresponding 1D Hamiltonian $$H(x,p)~=~\frac{p^2}{2m}+V(x)$$
always be finite?
The answer is in general No.
Counterexample:
$$V(x) ~=~ V_0 - \frac{A}{|x|^p},$$
where $V_0>0$ and $A>0$ are positive constants, and the power $p>2$. It is possible to prove that the spectrum is unbounded from below with infinitely many negative energy eigenstates in a very similar to e.g. methods used in this Phys.SE answer.
II)
What if one additionally assumes that the potential $V$ is bounded from below?
Then the answer is Yes, because there must exist positive constants $V_0,L>0$ such that
$$V(x)~\geq~ -V_0 ~\theta(L\!-\!|x|) .$$
In other words, one can find a finite potential well with lower energy levels, but we know that the spectrum of a finite potential well satisfies the sought-for statement.
III)
What if one instead only additionally assumes that the spectrum (but not necessarily the potential $V$) is bounded from below, i.e. that the system has a stable ground state?
Then the answer is Yes, semiclassically (WKB), and I believe it is Yes non-semiclassically as well, but I don't (yet) have a rigorous proof.