2405.06167
INTEGRABILITY-PRESERVING REGULARIZATIONS OF LAPLACIAN GROWTH
Razvan Teodorescu
correctmedium confidence
- Category
- Not specified
- Journal tier
- Note/Short/Other
- Processed
- Sep 28, 2025, 12:56 AM
- arXiv Links
- Abstract ↗PDF ↗
Audit review
The paper’s Section 3.3 defines the weak Laplacian Growth boundary as the zero set of ∂zΨ and explicitly notes that for classical times the boundary satisfies V′(z)+C_{μt}(z)=0, so that the gradient of Ψ vanishes exactly on ∂Ω(t) . It also states that weak solutions built from equilibrium measures persist beyond the critical time and are monotone in the sense K(s)⊆K(t), supp μ(s)⊆supp μ(t) , and remarks that on supp μt the tangential derivative of Ψ vanishes while the two normal limits are equal and opposite, cohering with the S-property picture used by the model solution . The candidate solution recovers these conclusions via potential-theoretic Euler–Lagrange/S-property methods and Gustafsson’s variational-inequality framework. It further adds standard details (meromorphic extension of Q² and quadratic differential trajectories) that the paper alludes to via branch-point/Riemann-surface data but does not spell out. Hence both are correct; the paper sketches the construction while the model provides a more detailed potential-theoretic route.
Referee report (LaTeX)
\textbf{Recommendation:} minor revisions \textbf{Journal Tier:} note/short/other \textbf{Justification:} This concise note proposes a weak, integrability-preserving formulation of Laplacian Growth via equilibrium measures and identifies the weak boundary as the zero set of the complex gradient of a potential-theoretic functional Ψ. The claims align with standard results and provide a coherent bridge to integrable-structures viewpoints. Minor clarifications on assumptions (external field regularity, boundary analyticity) and a brief explicit link from branch points to quadratic-differential trajectories would improve rigor and accessibility.