Abstract
We prove existence of infinitely many solutions u in H^1_r({mathbb {R}}^N) for the nonlinear Choquard equation -Δu+μu=(Iα∗F(u))f(u)inRN,\\documentclass[12pt]{minimal}\t\t\t\t\\usepackage{amsmath}\t\t\t\t\\usepackage{wasysym}\t\t\t\t\\usepackage{amsfonts}\t\t\t\t\\usepackage{amssymb}\t\t\t\t\\usepackage{amsbsy}\t\t\t\t\\usepackage{mathrsfs}\t\t\t\t\\usepackage{upgreek}\t\t\t\t\\setlength{\\oddsidemargin}{-69pt}\t\t\t\t\\begin{document}$$\\begin{aligned} - {\\varDelta } u + \\mu u =(I_\\alpha *F(u)) f(u) \\quad \\hbox {in}\\ {\\mathbb {R}}^N, \\end{aligned}$$\\end{document}where Nge 3, alpha in (0,N), I_alpha (x) := frac{{varGamma }(frac{N-alpha }{2})}{{varGamma }(frac{alpha }{2}) pi ^{N/2} 2^alpha } frac{1}{|x|^{N- alpha }}, x in {mathbb {R}}^N setminus {0} is the Riesz potential, and F is an almost optimal subcritical nonlinearity, assumed odd or even. We analyze the two cases: mu is a fixed positive constant or mu is unknown and the L^2-norm of the solution is prescribed, i.e. int _{{mathbb {R}}^N} |u|^2 =m>0. Since the presence of the nonlocality prevents to apply the classical approach, introduced by Berestycki and Lions (Arch Ration Mech Anal 82(4):347–375, 1983), we implement a new construction of multidimensional odd paths, where some estimates for the Riesz potential play an essential role, and we find a nonlocal counterpart of their multiplicity results. In particular we extend the existence results due to Moroz and Van Schaftingen (Trans Am Math Soc 367(9):6557–6579, 2015).
Highlights
Multiple solutions for the nonlinear Choquard equation with even or odd nonlinearities Silvia Cingolani1 · Marco Gallo1 · Kazunaga Tanaka2
375, 1983), we implement a new construction of multidimensional odd paths, where some estimates for the Riesz potential play an essential role, and we find a nonlocal counterpart of their multiplicity results
In [38, Theorem 1], they proved the existence of a ground state solution u ∈ H 1(RN ) of (1.1) and in [38, Theorem 4] they showed that, if F satisfies (F1), (F2) and, in addition, f is odd and has constant sign on (0, ∞), every ground state of (1.1) has constant sign and it is radially symmetric with respect to some point in RN
Summary
Multiple solutions for the nonlinear Choquard equation. Page 3 of 34 68 (1.2) represents the stationary nonlinear Hartree equation. In [38, Theorem 1], they proved the existence of a ground state solution u ∈ H 1(RN ) of (1.1) and in [38, Theorem 4] they showed that, if F satisfies (F1), (F2) and, in addition, f is odd and has constant sign on (0, ∞), every ground state of (1.1) has constant sign and it is radially symmetric with respect to some point in RN To our knowledge it is still an open problem the existence of infinitely many radially symmetric solutions for the nonlinear Choquard Eq (1.1) under the optimal assumptions (F1)–(F4) and symmetric conditions on the nonlocal source term (Iα ∗ F(u)) f (u).
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