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Maximum and antimaximum principles near the second eigenvalue. (English) Zbl 1240.35127

Summary: We consider the Dirichlet problem \(-\Delta u=\mu u+f\) in \(\Omega \), \(u=0\) on \(\partial \Omega \), with \(\Omega \) either a bounded smooth convex domain in \(\mathbb {R}^2\) or a ball or an annulus in \(\mathbb {R}^{N}\). Let \(\lambda _2\) be the second eigenvalue, with \(\varphi _2\) an associated eigenfunction. Although the two nodal domains of \(\varphi _2\) do not satisfy the interior ball condition, we are able to prove under suitable assumptions that, if \(\mu \) is sufficiently close to \(\lambda _2\), then the solution \(u\) of the above problem has also two nodal domains which appear as small deformations of the nodal domains of \(\varphi _2\). For \(N=2\) use is made in the proof of several results relative to the Payne conjecture.

MSC:

35J25 Boundary value problems for second-order elliptic equations
35B50 Maximum principles in context of PDEs
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