Abstract
We study here the Ginzburg-Landau functional on a Riemannian surface S endowed with an arbitrary metric
Eε(u)=½∫𝒮||∇u||2+1/(4ε2)∫𝒮(|u|2−1)2, u∈H1(S,C),
where ε∈]0,+∞[. We study the asymptotic behaviour of the critical points for Eε as ε→0. We define a renormalized energy which allows to characterize the position of the singularities at the limit.
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