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A note on a sinh-Poisson type equation with variable intensities on pierced domains

机译:关于SINH-POISSON类型方程的说明,穿孔域的可变强度

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We consider a sinh-Poisson type equation with variable intensities and Dirichlet boundary condition on a pierced domain Δ u + ρ ( V 1 ( x ) e u − V 2 ( x ) e − τ u ) = 0 in  Ω ϵ : = Ω ∖ ⋃ i = 1 m B ( ξ i , ϵ i ) ‾ u = 0 on  ∂ Ω ϵ , where ρ 0 , V 1 , V 2 0 are smooth potentials in Ω, τ 0 , Ω is a smooth bounded domain in R 2 and B ( ξ i , ϵ i ) is a ball centered at ξ i ∈ Ω with radius ϵ i 0 , i = 1 , … , m . When ρ 0 is small enough and m 1 ∈ { 1 , … , m − 1 } , there exist radii ϵ = ( ϵ 1 , … , ϵ m ) small enough such that the problem has a solution which blows-up positively at the points ξ 1 , … , ξ m 1 and negatively at the points ξ m 1 + 1 , … , ξ m as ρ → 0 . The result remains true in cases m 1 = 0 with V 1 ≡ 0 and m 1 = m with V 2 ≡ 0 , which are Liouville type equations.
机译:我们考虑一种Sinh-Poisson类型方程,穿孔域ΔU+ρ(V 1(x)eu-V 2(x)e-u)= 0,ωε:=ω∖ ⋃I= 1 m b(ξi,εi)〜u = 0°ωε,其中ρ& 0,v 1,v 2& 0是ω,τ&gt的光滑电位。 0,ω是r 2和b(νi,εi)中的平滑有界域是一个以ξi∈ω为中心的球,带半径εi& 0,i = 1,...,m。 当ρ& 0足够小,并且有M 1∈{1,...,m-1},存在半径ε=(ε1,...,εm)足够小,使得问题有一个溶液在点处积极爆发 1,...,ξM1和呈点ξm 1 + 1,...,ξm为ρ→0。 结果仍然是真的,其中m 1 = 0,V 1≠0和m 1 = m,V 2≠0,这是Liouville型方程。

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