Abstract

Abstract We consider the Hénon problem { - Δ ⁢ u = | x | α ⁢ u N + 2 + 2 ⁢ α N - 2 - ε in ⁢ B 1 , u > 0 in ⁢ B 1 , u = 0 on ⁢ ∂ ⁡ B 1 , \left\{\begin{aligned} &\displaystyle{-}\Delta u=\lvert x\rvert^{\alpha}u^{% \frac{N+2+2\alpha}{N-2}-\varepsilon}&&\displaystyle\phantom{}\text{in }B_{1},% \\ &\displaystyle u>0&&\displaystyle\phantom{}\text{in }B_{1},\\ &\displaystyle u=0&&\displaystyle\phantom{}\text{on }\partial B_{1},\end{% aligned}\right. where B 1 {B_{1}} is the unit ball in ℝ N {\mathbb{R}^{N}} and N ⩾ 3 {N\geqslant 3} . For ε > 0 {\varepsilon>0} small enough, we use α as a parameter and prove the existence of a branch of nonradial solutions that bifurcates from the radial one when α is close to an even positive integer.

Highlights

  • In this paper we consider the Henon problem−∆u = |x|αup in B1, u>0 in B1, (1) u = 0 on ∂B1.on the the unit ball B1 ⊂ RN with N 3, α > 0 and 1 < p < pα := N+N2−+22α

  • The equation (1) was introduced in [15] by Henon in the study of stellar cluster in spherically symmetric setting and it is known as Henon equation

  • We mention here some references but, since there is a vast literature regarding this problem and related ones, we remind that the list is far from complete

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Summary

Introduction

Similar ideas were used by Badiale and Serra [4] to obtain multiplicity results for some supercritical values of p and for α large Another approach to prove the existence of nonradial solutions is to use perturbation methods and the well known Lyapunov-Schimdt finite dimensional reduction. We consider the curve of radial solutions of (2) and α as a parameter, if ε is small enough there is a change in the Morse index of the radial solution of (2) for α close to an even integer and so we can apply the classical bifurcation theory to deduce the existence of a branch of nonradial solutions to the rescaled problem.

Properties of the radial solutions
The rescaled problem
The linearized problem
Proof of the main result
Full Text
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