Searcharxiv⌕ Search

arXiv · 2610.03091

Singular Contour Dynamics and Paradifferential Reduction

Abstract

We develop a direct paradifferential approach to nonlinear graph integral operators arising in contour dynamics. The main methodological result is an abstract structure-preserving paralinearization theorem, valid in arbitrary dimension, for a class of homogeneous kernels whose nonlinear dependence on the graph is expressed through normalized finite differences. The theorem covers both critical principal-value kernels and subcritical locally integrable kernels, gives explicit formulas for the principal symbols, and separates the finite-order symbolic contribution generated by the homogeneous singularity from order-zero far-field terms and arbitrarily smoothing remainders. A structural feature of the reduction is the cancellation of the intermediate symbolic order; at the critical endpoint the construction also preserves the exact skew-adjoint structure of the original singular integral. As a main application, we consider the three-dimensional two-phase free-boundary Euler equations with constant interfacial background vorticity. We first derive an autonomous contour-dynamics equation in canonical surface variables and then apply the abstract theorem directly to the singular integral operators generated by the Birkhoff--Rott formulation. This yields the complete paradifferential structure of the system without taking the Dirichlet--Neumann reduction as a starting point. After introducing an Alinhac good unknown and diagonalizing the resulting system, we obtain local well-posedness for small Sobolev perturbations in the stable Kelvin--Rayleigh--Taylor regime, uniformly on compact subsets of the stable parameter set.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Xingyu Li, Emeric Roulley, Stefano Scrobogna. 2026-10-02. Singular Contour Dynamics and Paradifferential Reduction. https://arxiv.org/abs/2610.03091

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Global-in-time Well-posedness of Classical Solutions to the Vacuum Free Boundary Problem for the 1-D Viscous Saint-Venant System with Large Data

We establishes the global existence and uniqueness of classical solutions to the vacuum free boundary problem for the 1-D viscous Saint-Venant system with a general class of large initial data. Since the fluid depth $ρ$ vanishes on the moving boundary, the momentum equations degenerate in both time evolution and spatial dissipation, potentially causing singularities in velocity derivatives and making classical solutions difficult to construct. By exploiting the intrinsic degenerate-singular structures, we identify admissible initial depth profiles for which $ρ_0^α$ belongs to $H^3$ and vanishes as the distance to the moving boundary, with $\frac{1}{3}<α\le 1$. In particular, for $α=1$, it satisfies the physical vacuum boundary condition but violates the BD entropy condition. First, we introduce new weighted nonlinear energy functionals involving lower- and higher-order derivatives, based on the balance between pressure and spatial dissipation. Second, we derive new global weighted $L^p$ estimates, $2\le p\le\infty$, for the effective velocity $v=u+(\logρ)_y$, where $y$ is the Eulerian coordinate, using the transport properties of its evolution equation. These estimates differ from those of Bresch-Desjardins (Comm. Math. Phys. 238 (2003), 211-223) and Kanel (Differ. Uravn. 4 (1968), 721-734) and are crucial for $α=1$, where the BD entropy condition fails. Finally, we establish weighted energy estimates for first-order velocity derivatives with weights involving powers of $ρ_0$ and $η_x$, where $x$ is the Lagrangian coordinate and $η$ the flow map. These estimates give an upper bound for $η_x$ on every finite time interval without any smallness assumption on the initial data. Further singular or degenerate weighted energy estimates yield the desired global regularity.

math.AP↗

Desingularization of vortex sheets for the 2D Euler equations

We show how to regularize vortex sheets by means of smooth, compactly supported vorticities that asymptotically evolve according to the Birkhoff-Rott vortex sheet dynamics. More precisely, consider a vortex sheet initial datum $ω^0_{\mathrm{sing}}$, which is a signed Radon measure supported on a closed curve. We construct a family of initial vorticities $ω^0_\varepsilon \in C^\infty_c(\mathbb{R}^2)$ converging to $ω^0_{\mathrm{sing}}$ distributionally as $\varepsilon \to 0^+$, and show that the corresponding solutions $ω_\varepsilon(x,t)$ to the 2D incompressible Euler equations converge to the measure defined by the Birkhoff-Rott system with initial datum $ω^0_{\mathrm{sing}}$. The regularization relies on a layer construction designed to exploit the key observation that the Kelvin-Helmholtz instability has a strongly anisotropic effect: while vorticities must be analytic in the "tangential" direction, the way layers can be arranged in the "normal" direction is essentially arbitrary.

math.AP↗

Global-in-time convergence from bipolar Euler-Poisson equations to unipolar ones

In this paper, the Cauchy problem for the multi-dimensional (M-D) bipolar Euler-Poisson equations with far field vacuum is considered. Based on physical observations and some elaborate analysis of this system's intrinsic structures, for a class of smooth initial data that are of small scaled density but possibly large mean velocity, we give one rigorous global-in-time convergence proof for regular solutions from M-D bipolar Euler-Poisson equations to M-D unipolar Euler-Poisson equations through the vanishing electron-to-ion mass-ratio limit. Here the initial scaled density is required to vanish in the far field, and the spectrum of the Jacobian matrix of the initial mean velocity stays uniformly away from the nonpositive real axis. In order to deal with singular limits of this kind, the global-in-time uniform tame estimates of regular solutions to M-D bipolar Euler-Poisson equations with respect to the mass ratio are established, based on which the corresponding error estimates in smooth function spaces between the two systems considered are given. To this end, we establish global a priori estimates for solutions with compactly supported initial densities, uniformly in the mass ratio and the initial support radii. Compactness then yields global regular solutions for general initial densities.

math.AP↗