The resolvent for Laplace-type operators on asymptotically conic spaces

Andrew Hassell[1]; András Vasy[2]

  • [1] Australian National University, Centre for Mathematics and its Applications, Canberra ACT 0200 (Australie)
  • [2] Massachusetts Institute of Technology, Department of Mathematics, Cambridge MA (USA)

Annales de l’institut Fourier (2001)

  • Volume: 51, Issue: 5, page 1299-1346
  • ISSN: 0373-0956

Abstract

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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 = Δ + P , where Δ is the Laplacian with respect to g and P is a self-adjoint first order scattering differential operator with coefficients vanishing at 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 ( σ + i 0 ) , for σ 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.

How to cite

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Hassell, Andrew, and Vasy, András. "The resolvent for Laplace-type operators on asymptotically conic spaces." Annales de l’institut Fourier 51.5 (2001): 1299-1346. <http://eudml.org/doc/115949>.

@article{Hassell2001,
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.},
affiliation = {Australian National University, Centre for Mathematics and its Applications, Canberra ACT 0200 (Australie); Massachusetts Institute of Technology, Department of Mathematics, Cambridge MA (USA)},
author = {Hassell, Andrew, Vasy, András},
journal = {Annales de l’institut Fourier},
keywords = {Legendre distributions; symbol calculus; scattering metrics; resolvent kernel},
language = {eng},
number = {5},
pages = {1299-1346},
publisher = {Association des Annales de l'Institut Fourier},
title = {The resolvent for Laplace-type operators on asymptotically conic spaces},
url = {http://eudml.org/doc/115949},
volume = {51},
year = {2001},
}

TY - JOUR
AU - Hassell, Andrew
AU - Vasy, András
TI - The resolvent for Laplace-type operators on asymptotically conic spaces
JO - Annales de l’institut Fourier
PY - 2001
PB - Association des Annales de l'Institut Fourier
VL - 51
IS - 5
SP - 1299
EP - 1346
AB - 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.
LA - eng
KW - Legendre distributions; symbol calculus; scattering metrics; resolvent kernel
UR - http://eudml.org/doc/115949
ER -

References

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  10. R. B. Melrose, Spectral and scattering theory for the Laplacian on asymptotically Euclidian spaces, (1994), Marcel Dekker Zbl0837.35107MR1291640
  11. R. B. Melrose, G. Uhlmann, Lagrangian Intersection and the Cauchy problem, Comm. Pure and Appl. Math. 32 (1979), 483-519 Zbl0396.58006MR528633
  12. R. B. Melrose, M. Zworski, Scattering metrics and geodesic flow at infinity, Inventiones Mathematicae 124 (1996), 389-436 Zbl0855.58058MR1369423
  13. A. Vasy, Geometric scattering theory for long-range potentials and metrics, Int. Math. Res. Notices (1998), 285-315 Zbl0922.58085MR1616722
  14. J. Wunsch, M. Zworski, Distribution of resonances for asymptotically euclidean manifolds Zbl1030.58024MR1849026

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