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)
Summary
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.
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