How statement and proof provenance work
The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.
- Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
- AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
- AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.
These labels describe origin, not correctness: citations and verification chips remain separate evidence.
Unique continuation for general non-trapping obstacles and trajectories
PDF p. 21: §5.2(A)
Open problem
Assume the Axiom of Choice: every family of nonempty sets admits a choice function. Let , , and . Let be a nonempty compact obstacle with smooth boundary, connected exterior , and the non-trapping property of Non-trapping obstacle. For any with , put .
For every reference trajectory satisfying (W) as defined in Reference trajectory hypothesis W, does (UCPw), as defined in Conditional energy-level unique continuation hypothesis, hold for this and ? Explicitly, does every satisfying in distributions on and vanishing almost everywhere on vanish identically as an -valued path?
Status
The frozen article, §5.2(A), reports this question open for general trajectories and non-trapping obstacles. It notes that the coefficients can depend on time and need not be analytic, and proposes Carleman estimates as a possible approach while noting that known approaches commonly impose additional geometry. This is attribution of the authors' status and suggested approach, not a proof that the question remains open worldwide.
A related result of Filippas, Laurent and Léautaud treats Schrödinger operators with lower-order coefficients Gevrey 2 in time; their Theorem 1.7 concerns a scalar equation on the unit disk under additional hypotheses. These conditions and that scalar setting do not establish the question above for the conjugate-coupled equation and arbitrary (W) trajectories. A limited literature search on 2026-11-13 did not identify a solution covering the complete stated formulation; it is not an exhaustive current-status review.
Depends on
- Reference trajectory hypothesis W
- Conditional energy-level unique continuation hypothesis
- Non-trapping obstacle
- The Axiom of Choice
- Unique continuation for Schrödinger operators with partially Gevrey coefficients · Author manuscript dated 31 March 2025: abstract, PDF p. 1; Section 1.2, equation (1.18), Theorem 1.7 and equation (1.19), PDF pp. 6–7.
Dependency tree · 2 levels
Each result is drawn at its shortest distance from this item. Arrows run from prerequisites to the items that use them; this item has a heavier outline. External source nodes link directly to the cited text. The view shows up to two dependency steps; open a prerequisite to continue.
External dependencies
The abstract gives local unique continuation for Schrödinger operators with time-independent Lipschitz metric and lower-order coefficients Gevrey 2 in time and bounded in space. For the scalar Dirichlet equation i partial_t u + Delta u + q u = 0 on the Euclidean unit disk, Theorem 1.7 states that for every T > 0 there is C > 0 such that the squared initial L2 norm is at most C times the integral of |u| squared over (0,T) times omega.
Hypotheses: For Theorem 1.7, the manifold is the closed Euclidean unit disk D; q is real-valued and belongs to C-infinity([0,T] times D) intersected with G2((0,T); L-infinity-loc(Int D)); omega is a nonempty relatively open subset of D meeting its boundary; the solution of (1.18) has homogeneous Dirichlet boundary condition and initial datum in L2(D). The abstract has the separate metric and coefficient assumptions stated in the statement field.
Reading limits: This maintenance turn read the abstract and Section 1.2, including (1.18), Theorem 1.7, (1.19), and the discussion immediately following it, in the author-hosted CNRS manuscript. The proof and the cited high-frequency result ALM16 were not reconstructed. This scalar disk result is contextual: no application to the conjugate-coupled exterior adjoint equation or arbitrary (W) trajectories is claimed, and no exhaustive worldwide status survey was performed.
Sources
- Nonlinear Schrödinger equation in an exterior domain, v2 · PDF page 21, §5.2(A); PDF pages 4–5, hypotheses (W) and (UCPw)
- Unique continuation for Schrödinger operators with partially Gevrey coefficients · Author manuscript dated 31 March 2025: abstract, PDF p. 1; Section 1.2, equation (1.18), Theorem 1.7 and equation (1.19), PDF pp. 6–7.