The Ozawa solution to the Davey--Stewartson II equations and surface theory
Yi C. Huang, Iskander A. Taimanov
TL;DR
The paper establishes a geometric interpretation of the Ozawa blow-up solution to the Davey--Stewartson II equation by formulating a soliton deformation of Weierstrass-type surfaces via a pseudo-conformal transformation. Starting from a stationary radial potential $U=\frac{1}{1+z\bar z}$, the authors apply the pseudo-conformal map to obtain the Ozawa solution $\widetilde{U}$ and compute the associated transformed spinors, yielding an explicit surface deformation in ${\mathbb R}^3\subset{\mathbb R}^4$ with $x^4=0$. The resulting coordinates satisfy $w_1=\frac{it^2 z}{t^2+|z|^2}$ and $w_2=\frac{-t^3}{t^2+|z|^2}$, which collapse to zero as $t\to0$ for $z\neq0$, providing a concrete geometric counterpart to the Ozawa singularity. The work clarifies the relationship between DSII blow-up phenomena and surface theory, highlighting differences from indeterminacy-type solutions and offering a geometric lens on singularity formation in integrable systems.
Abstract
We describe the Ozawa solution to the Davey--Stewartson II equation from the point of view of surface theory by presenting a soliton deformation of surfaces which is ruled by the Ozawa solution. The Ozawa solution blows up at certain moment and we describe explicitly the corresponding singularity of the deformed surface.
