On the resonant Lane-Emden problem for the p-Laplacian

preprint2012arXivOpen access

Abstract

We study the positive solutions of the Lane-Emden equation −Δpu=λp∣u∣q−2u-Δ_{p}u=λ_{p}|u|^{q-2}u in ΩΩ with homogeneous Dirichlet boundary conditions, where Ω⊂RNΩ\subset\mathbb{R}^{N} is a bounded and smooth domain, N≥2,N\geq2, λpλ_{p} is the first eigenvalue of the pp-Laplacian operator ΔpΔ_{p} and qq is close to p>1.p>1. We prove that any family of positive solutions of this problem converges in C1(Ωˉ)C^{1}(\barΩ) to the function θpepθ_{p}e_{p} when q→p,q\rightarrow p, where epe_{p} is the positive and L∞L^{\infty}-normalized first eigenfunction of the pp-Laplacian and θp:=exp⁡(∣ep∣Lp(Ω)−p∫Ωepθ_{p}:=\exp(|e_{p}|_{L^{p}(Ω)}^{-p}\int_Ωe_{p}% ^{p}|\ln e_{p}|dx). A consequence of this result is that the best constant of the immersion W01,p(Ω)↪Lq(Ω)W_{0}^{1,p}(Ω)\hookrightarrow L^{q}(Ω) is differentiable at q=p.q=p. Previous results on the asymptotic behavior (as q→pq\rightarrow p) of the positive solutions of the non-resonant Lane-Emden problem (i.e. with λpλ_{p} replaced by a positive λ≠λpλ\neqλ_{p}) are also generalized to the space C1C^{1}% (\barΩ) and to arbitrary families of these solutions. Moreover, if uλ,qu_{λ,q} denotes a solution of the non-resonant problem for an arbitrarily fixed λ>0,λ>0, we show how to obtain the first eigenpair of the pp-Laplacian as the limit in C1(Ωˉ),C^{1}(\barΩ), when q→pq\rightarrow p, of a suitable scaling of the pair (λ,uλ,q).(λ,u_{λ,q}). For computational purposes the advantage of this approach is that λλ does not need to be close to λp.λ_{p}. Finally, an explicit estimate involving L∞L^{\infty} and L1L^{1} norms of uλ,qu_{λ,q} is also deduced using set level techniques.

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