Alphabeta Math
Open problemQuestion: Literature-sourcedProof: Not applicable
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 n≥2, T>0, and λ∈R∖{0}. Let Θ⊂Rn be a nonempty compact obstacle with smooth boundary, connected exterior Ω=Rn∖Θ, and the non-trapping property of Non-trapping obstacle. For any R>0 with Θ⊂BR(0), put ω={x∈Ω:∣x∣>R}.

For every reference trajectory w satisfying (W) as defined in Reference trajectory hypothesis W, does (UCPw), as defined in Conditional energy-level unique continuation hypothesis, hold for this T and ω? Explicitly, does every v∈C([0,T];H01(Ω)) satisfying i∂tv+Δv+2λ∣w∣2v−λw2v‾=0 in distributions on (0,T)×Ω and vanishing almost everywhere on (0,T)×ω vanish identically as an H01(Ω)-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

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

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.

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