Bifurcation into spectral gaps for strongly indefinite Choquard equations

preprint2022arXivOpen access

Abstract

We consider the semilinear elliptic equations {−Δu+V(x)u=(Iα∗∣u∣p)∣u∣p−2u+λufor x∈RN,u(x)→0 as ∣x∣→∞, \left\{ \begin{array}{ll} &-Δu+V(x)u=\left(I_α\ast |u|^p\right)|u|^{p-2}u+λu\quad \hbox{for } x\in\mathbb R^N, \\ &u(x) \to 0 \hbox{ as } |x| \to\infty, \end{array} \right. where IαI_α is a Riesz potential, p∈(N+αN,N+αN−2)p\in(\frac{N+α}N,\frac{N+α}{N-2}), N≥3N\geq3, and VV is continuous periodic. We assume that 00 lies in the spectral gap (a,b)(a,b) of −Δ+V-Δ+ V. We prove the existence of infinitely many geometrically distinct solutions in H1(RN)H^1(\mathbb R^N) for each λ∈(a,b)λ\in(a, b), which bifurcate from bb if N+αN<p<1+2+αN\frac{N+α}N< p < 1 +\frac{2+α}{N}. Moreover, bb is the unique gap-bifurcation point (from zero) in [a,b][a,b]. When λ=aλ=a, we find infinitely many geometrically distinct solutions in Hloc2(RN)H^2_{loc}(\mathbb R^N). Final remarks are given about the eventual occurrence of a bifurcation from infinity in λ=aλ=a.

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