The resolvent for Laplace-type operators on asymptotically conic spaces
Andrew Hassell and András Vasy
Abstract:
Let $X$ be a compact manifold with boundary, and $g$ a
scattering metric on $X$, which may be either of short range or `gravitational'
long range type. Thus, $g$ gives $X$ the geometric structure of a complete
manifold with an asymptotically conic end.
Let $H$ be an operator of the form $H =
\Delta + P$, where $\Delta$ is the Laplacian with respect to $g$ and
$P$ is a self-adjoint first order scattering differential operator with
coefficients vanishing at $\partial X$ and satisfying a `gravitational'
condition. We define a symbol calculus for Legendre distributions on
manifolds with codimension two corners and use it to give a
direct construction of the resolvent kernel of $H$, $R(\sigma + i0)$, for
$\sigma$ on the positive real axis.
In this approach, we do not use the limiting
absorption principle at any stage; instead we construct a parametrix
which solves the resolvent equation up to a compact error term and then use
Fredholm theory to remove the error term.