2501.06796
Conefield approach to identifying regions without flux surfaces for magnetic fields
D. Martínez-del-Río, R. S. MacKay
correctmedium confidence
- Category
- Not specified
- Journal tier
- Specialist/Solid
- Processed
- Sep 28, 2025, 12:56 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper states the conefield Converse KAM nonexistence criterion (Theorem 3.1) using the same objects and hypotheses as the candidate solution: α0 = iB iξ Ω ≡ (ξ×B)♭, its pullbacks αt = ϕt*α0, the slope σt = αt(η)/αt(ξ), and the condition that there exist times t± with ±αt±(ξ)>0 and σt+ ≤ σt− implying no invariant torus transverse to ξ through x0. The paper summarizes the argument and procedure without a detailed proof, while the candidate solution gives a clean contradiction proof via the inequality αt(ξ)(σt−s*)>0 built from the torus’ horizontal tangent direction w0=η−s*ξ. This is the standard cone-field reasoning underpinning Theorem 3.1 and matches the paper’s construction and definitions, hence both are correct and essentially the same proof in content, with the model providing the missing detailed steps. See the theorem statement and setup in the paper (slope/order definitions, α0 choice, and Theorem 3.1) .
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions \textbf{Journal Tier:} specialist/solid \textbf{Justification:} The paper correctly reformulates and implements a well-established Converse KAM nonexistence criterion via conefields for magnetic fields. The main theorem is stated accurately and the numerical implementation is useful. However, Theorem 3.1 is presented as a summary without a proof; adding a compact proof sketch or a precise reference to a proof would improve completeness. Clarifications on assumptions and edge cases (shearless) would further strengthen the presentation.