Abstract

We consider the question of whether solutions of Klein–Gordon equations on asymptotically anti-de Sitter spacetimes can be uniquely continued from the conformal boundary. Positive answers were first given in [, ], under suitable assumptions on the boundary geometry and with boundary data imposed over a sufficiently long timespan. The key step was to establish Carleman estimates for Klein–Gordon operators near the conformal boundary. In this article, we further improve upon the above-mentioned results. First, we establish new Carleman estimates—and hence new unique continuation results—for Klein–Gordon equations on a larger class of spacetimes than in [, ], in particular with more general boundary geometries. Second, we argue for the optimality, in many respects, of our assumptions by connecting them to trajectories of null geodesics near the conformal boundary; these geodesics play a crucial role in the construction of counterexamples to unique continuation. Finally, we develop a new covariant formalism that will be useful—both presently and more generally beyond this article—for treating tensorial objects with asymptotic limits at the conformal boundary.

Highlights

  • We revisit the problem of unique continuation for Klein–Gordon equations from the conformal boundary of asymptotically Anti-de Sitter spacetimes

  • (5) We develop a general formalism of vertical tensor fields to treat the relevant tensorial quantities in our spacetime that have asymptotic limits at the conformal boundary

  • The first theorem is a Carleman estimate for Klein–Gordon operators, assuming the null convexity criterion (1.11) and (1.12); this directly leads to unique continuation results for (1.4)

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Summary

Introduction

We revisit the problem of unique continuation for Klein–Gordon equations from the conformal boundary of asymptotically Anti-de Sitter spacetimes. In Theorem 1.14, one assumes φ vanishes on an entire time slab {t0 ≤ t ≤ t1} of the conformal boundary It is not yet clear whether similar Carleman estimates or unique continuation results hold with vanishing on regions D ⊆ I that are spatially localized. (The is based on a projective geometric argument in the unique continuation literature for wave operators; see [27].) From this point, arguments similar to those in [16] allow us to construct a family of hypersurfaces that are pseudoconvex near the conformal boundary Another key aspect is the use of a Riemannian metric h to measure the sizes of vertical tensor fields.

Asymptotically AdS Spacetimes
The Null Convexity Criterion
Null Geodesics
The Carleman Estimate

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