Let $T:=-\frac{d^2}{dx^2}$ on $C_c^{\infty}(0,1) \subset L^2(0,1),$ then I know that $T^*$ is defined on $H^2(0,1).$ What happens now if I consider instead $T+V$ where $V \in L^2(0,1)$? Is this implication then still true? Obviously, we have $(T+V)^* \supset T^*+V^*$ where the right hand side is defined on $H^2(0,1).$ Does the converse implication hold in general as well?
I don't know if it helps, but $L^2$ potentials are relatively $0-$bounded w.r.t. the second derivative.