Set $ A_i:= -\Delta + V_i :H^2(\mathbb{R}^3) \subseteq L^2(\mathbb{R}^3) \to L^2(\mathbb{R}^3), \ i =1,2 $, where \begin{equation*} V_1 = 0, \ \ (\textrm{No interaction}) \\ V_2 = - \frac{\gamma}{\vert x \vert}, \gamma >0, \ \ (\textrm{Coulumb potential}). \end{equation*} By the fact that $ 0 \in \sigma_c(A_i), \ i =1,2 $,
Remark: This result could be found in Chapter 7, 10 in "G. Teschl: Mathematical Methods in Quantum Mechanics - With Applications to Schrödinger Operators (2014)".
we know \begin{equation*} \mathcal{N}(A_i) = 0, \ \overline{\mathcal{R}(A_i)} = L^2(\mathbb{R}^3) \\ \ A^{-1}_i \ \textrm{unbounded} \ (i =1,2) \end{equation*} Question: Can we find a bounded restriction for $ A^{-1}_i $, that is, there exist $ \mathcal{B}_i \subseteq \mathcal{R}(A_i) $ such that $ A^{-1}_i|_{\mathcal{B}_i} $ are bounded respectively?
Good references will be welcome. Thank you in advance!
Notice: This question is highly related to (Non-closed range space of Laplace operators?) and ($ 0 $ locates in the continuous spectrum of Schrodinger operators?).