Weakly regular T2 symmetric spacetimes. The future causal geometry of Gowdy spaces
Philippe G. LeFloch, Jacques Smulevici

TL;DR
This paper studies the future causal structure of weakly regular Gowdy spacetimes on T3, proving they are future causally geodesically complete and extending previous results to lower regularity settings.
Contribution
It establishes future causal geodesic completeness for Gowdy spacetimes with weak regularity, using novel energy decay and geodesic analysis methods.
Findings
Proves weakly regular Gowdy spacetimes are future causally geodesically complete.
Extends Ringström's theorem to lower regularity metrics.
Provides an alternative, shorter proof of energy decay and geodesic completeness.
Abstract
We investigate the future asymptotic behavior of Gowdy spacetimes on T3, when the metric satisfies weak regularity conditions, so that the metric coefficients (in suitable coordinates) are only in the Sobolev space H1 or have even weaker regularity. The authors recently introduced this class of spacetimes in the broader context of T2 symmetric spacetimes and established the existence of a global foliation by spacelike hypersurfaces when the time function is chosen to be the area of the surfaces of symmetry. In the present paper, we identify the global causal geometry of these spacetimes and, in particular, establish that weakly regular Gowdy spacetimes are future causally geodesically complete. This result extends a theorem by Ringstr\"om for metrics with sufficiently high regularity. We emphasize that our proof of the energy decay is based on an energy functional inspired by the…
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
Taxonomy
TopicsGeometric Analysis and Curvature Flows · Geometry and complex manifolds · Geometric and Algebraic Topology
