Asymptotic behavior of least energy solutions for a biharmonic problem with nearly critical growth

Asymptotic behavior of least energy solutions for a biharmonic problem with nearly critical growth
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DOI:
10.3233/asy-2008-0904
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发表时间:
2009-02
期刊:
Asymptot. Anal.
影响因子:
--
通讯作者:
F. Takahashi
F. Takahashi
中科院分区:
其他
文献类型:
--
作者:
F. Takahashi

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当ε → +0时,其中Ω是RN(N5)中的光滑有界区域,c 0 =(N − 4)(N − 2)N(N + 2),ε > 0是一个小的正参数,pε = p − ε,p =(N + 4)/(N − 4)是从Sobolev嵌入H2 → Lp+1(Ω)的观点看的临界Sobolev指数,且K ∈ C2(Ω)是给定的正函数。(Pε,K)的边界条件称为Navier边界条件。对于二阶Laplacian情形的问题ε n = N(N − 2)K(x)u(N+2)/(N −2)−ε in Ω,u > 0 in Ω,u = 0 on Ω,
as ε → +0, where Ω is a smooth bounded domain in RN (N 5), c0 = (N − 4)(N − 2)N (N + 2), ε > 0 is a small positive parameter, pε = p − ε, p = (N + 4)/(N − 4) is the critical Sobolev exponent from the view point of the Sobolev embedding H2 ∩ H1 0 (Ω) ↪→ Lp+1(Ω), and K ∈ C2(Ω) is a given positive function. Boundary condition of (Pε,K) is called as the Navier boundary condition. For the second-order Laplacian-case problem ⎧⎨ ⎩ −Δu = N (N − 2)K(x)u(N+2)/(N −2)−ε in Ω, u > 0 in Ω, u = 0 on ∂Ω,