Abstract
We consider the following Chern-Simons equation, \begin{equation} \label{0.1} Δu+\frac 1{\varepsilon^2} e^u(1-e^u)=4π\sum_{i=1}^N δ_{p_i^\varepsilon},\quad \text{in}\quad Ω, \end{equation} where is a 2-dimensional flat torus, is a coupling parameter and stands for the Dirac measure concentrated at . In this paper, we proved that the topological solutions of \eqref{0.1} are uniquely determined by the location of their vortices provided the coupling parameter is small and the collapsing velocity of vortices is slow enough or fast enough comparing with . This extends the uniqueness results of Choe \cite{Choe2005} and Tarantello \cite{Tarantello2007}. Meanwhile, for any topological solution defined in whose linearized operator is non-degenerate, we construct a sequence topological solutions of \eqref{0.1} whose asymptotic limit is exactly after rescaling around . A consequence is that non-uniqueness of topological solutions in implies non-uniqueness of topological solutions on torus with collapsing vortices.
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