Solutions of the Ginzburg-Landau equations concentrating on codimension-2 minimal submanifolds (2211.03131v1)
Abstract: We consider the magnetic Ginzburg-Landau equations in a compact manifold $N$ $$ \begin{cases} -\varepsilon2 \Delta{A} u=\frac{1}{2}(1-|u|2)u,\ \varepsilon2 d*dA=\langle\nablaA u,iu\rangle \end{cases} $$ formally corresponding to the Euler-Lagrange equations for the energy functional $$ E(u,A)=\frac{1}{2}\int_{N}\varepsilon2|\nablaAu|{2}+\varepsilon4|dA|{2}+\frac{1}{4}(1-|u|{2}){2}. $$ Here $u:N\to \mathbb{C}$ and $A$ is a 1-form on $N$. Given a codimension-2 minimal submanifold $M\subset N$ which is also oriented and non-degenerate, we construct a solution $(u_\varepsilon,A_\varepsilon)$ such that $u_\varepsilon$ has a zero set consisting of a smooth surface close to $M$. Away from $M$ we have $$ u_\varepsilon(x)\to\frac{z}{|z|},\quad A_\varepsilon(x)\to\frac{1}{|z|2}(-z2dz1+z1dz2),\quad x=\exp_y(z\beta\nu_\beta(y)). $$ as $\varepsilon\to 0$, for all sufficiently small $z\ne 0$ and $y\in M$. Here, ${\nu_1,\nu_2}$ is a normal frame for $M$ in $N$. This improves a recent result by De Philippis and Pigati who built a solution for which the concentration phenomenon holds in an energy, measure-theoretical sense.