# Resolvents of Schrodinger operators

In the free case one can compute the resolvents of the Laplacian $-\Delta$ in many cases explicitly, in the sense that they are given by an integral operator. Often, one uses the Hille-Yosida theorem or Fourier transform to do so.

Also, the Schwartz-kernel theorem tells us that in a distributional sense there is always an "integral kernel" associated to the resolvent of a Schrodinger operator.

However, examples in the free case suggest that the resolvent of $H:=-\frac{d^2}{dx^2} +V$ ( I am now in dimension $1$ as I would just like to get some conceptual insight) where $V$ is a $C^{\infty}$ and bounded potential with suitable boundary conditions such that this operator is self-adjoint, gives rise to a resolvent

$$(H-z)^{-1}\psi(x) = \int K_z(x,y)\psi(y) dy$$ where $K_z$ has, for fixed $z$ in the resolvent set, nice properties (almost always smooth) in $x$ and $y$.

See for example this calculation: of the one-dimensional resolvent or this one of the three-dimensional on math.stackexchange

I would like to ask why this is the case? Which theorem guarantees us that such nice $K_z$ kernels exist?

There is a general answer for any dimension $n\geq1$. Let $\Omega\subseteq \mathbb R^n$ denote the underlying domain.
For all $z$ in the resolvent set of $H$, $(H-z)^{-1}$ is a (classical) pseudodifferential operator of order $-2$, as $-\Delta+V$ is elliptic. Hence, its kernel $K_z$ is a distribution on $\Omega\times\Omega$ which is conormal with respect to the diagonal $\Delta_\Omega = \{(x,x)\mid x\in\Omega\}$. This implies that the wave front set of $K_z$ is contained in the conormal bundle $N^\ast \Delta_\Omega\setminus0 = \{(\xi,-\xi)\in T_{(x,x)}^*(\Omega\times\Omega)\mid x\in\Omega,\,$ $\xi\in T_x^*\Omega\setminus0\}$. In particular, its singular support is contained in (actually, it is equal to) $\Delta_\Omega$.
Further properties of the kernel $K_z$ depend on the situation under consideration. For instance, if $\Omega$ is bounded and smooth and $V$ is smooth up to the boundary, then $(H-z)^{-1}$ belongs to Boutet de Monvel's calculus, see e.g. Gerd Grubb Functional calculus of pseudodifferential boundary problems. For $\Omega=\mathbb R^n$, there are (refined) pseudodifferential calculi adapted to the behavior of the potential $V$ as $|x|\to\infty$.