When reading the paper Control for Schrödinger operators on tori by N.Burq and M.Zworski (Math. Res. Lett., 19(2):309–324, 2012), an inequality confused me:
Define the flat torus $\mathbb{T}^2=\mathbb{R}^2/A\mathbb{Z}\times B\mathbb{Z}$. Suppose $u_0\in L^2(\mathbb{T}^2)$. $\Delta$ is the Laplace operator and $V\in\mathcal{C}^\infty(\mathbb{T}^2)$ is a smooth potential.
We define $$ v_{\varepsilon,0}=\frac{1}{\varepsilon} \left(e^{-i\varepsilon(-\Delta+V)}-I \right) u_0. $$ We can write $u_0$ in terms of orthonormal eigenvectors of Schrödinger operator $-\Delta+V: u_0=\sum_{\lambda\in\sigma(-\Delta+V)}u_{0,\lambda}e_\lambda$, then we have $$ \left \| v_{0,\alpha}-v_{0,\beta} \right \| _{H^{-4}}^2 \leq \sum_{\lambda\in\sigma(-\Delta+V)} \left | \frac{e^{-i\alpha \lambda}-1}{\alpha}-\frac{e^{-i\beta \lambda}-1}{\beta} \right | ^2 (1+\lambda)^{-2}\left | u_{0,\lambda} \right |^2. $$ What confused me is the term $(1+\lambda)^{-2}$.
I know the definition of the norm $\left \| u_0 \right \| _{H^{-4}}=\left \| (1-\Delta)^{-2}u_0 \right \|_{L^2}$, but what is the relationship between the eigenvalues of $-\Delta$ and $-\Delta+V$?
Why we can "substitute" the eigenvalues of $-\Delta+V$ into the position of $-\Delta$?
Thanks in advance!