Solutions with Vortices of a Semi-Stiff Boundary Value Problem for the Ginzburg-Landau Equation

TL;DR

This paper demonstrates the existence of stable vortex solutions near the boundary for a semi-stiff boundary problem in the 2D Ginzburg-Landau equation, using a novel variational approach with an approximate bulk degree.

Contribution

It introduces a variational method with an approximate bulk degree to construct stable vortex solutions under semi-stiff boundary conditions, extending understanding beyond known Dirichlet cases.

Findings

Stable solutions with boundary vortices exist with bounded energy as epsilon approaches zero.

The method constructs local energy minimizers using a new approximate bulk degree.

Nonexistence of such solutions is proved for simply connected domains under Neumann conditions.

Abstract

We study solutions of the 2D Ginzburg-Landau equation -\Delta u+\frac{1}{\ve^2}u(|u|^2-1)=0 subject to "semi-stiff" boundary conditions: the Dirichlet condition for the modulus, |u|=1, and the homogeneous Neumann condition for the phase. The principal result of this work shows there are stable solutions of this problem with zeros (vortices), which are located near the boundary and have bounded energy in the limit of small epsilon. For the Dirichlet bondary condition ("stiff" problem), the existence of stable solutions with vortices, whose energy blows up as epsilon goes to 0, is well known. By contrast, stable solutions with vortices are not established in the case of the homogeneous Neumann ("soft") boundary condition. (nonexistence is proved for simply connected domains). In this work, we develop a variational method which allows one to construct local minimizers of the corresponding Ginzburg-Landau energy functional. We introduce an approximate bulk degree as the key ingredient of this method, and, unlike the standard degree over the curve, it is preserved in the weak H^1-limit.