114 research outputs found

    Low energy solutions for singularly perturbed coupled nonlinear systems on a Riemannian manifold with boundary

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    Let (M,g) be asmooth, compact Riemannian manifold with smooth boundary, with n= dim M= 2,3. We suppose the boundary of M to be a smooth submanifold of M with dimension n-1. We consider a singularly perturbed nonlinear system, namely Klein-Gordon-Maxwell-Proca system, or Klein-Gordon-Maxwell system of Scrhoedinger-Maxwell system on M. We prove that the number of low energy solutions, when the perturbation parameter is small, depends on the topological properties of the boundary of M, by means of the Lusternik Schnirelmann category. Also, these solutions have a unique maximum point that lies on the boundary

    Nodal solutions for the Choquard equation

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    We consider the general Choquard equations Δu+u=(Iαup)up2u -\Delta u + u = (I_\alpha \ast |u|^p) |u|^{p - 2} u where IαI_\alpha is a Riesz potential. We construct minimal action odd solutions for p(N+αN,N+αN2)p \in (\frac{N + \alpha}{N}, \frac{N + \alpha}{N - 2}) and minimal action nodal solutions for p(2,N+αN2)p \in (2,\frac{N + \alpha}{N - 2}). We introduce a new minimax principle for least action nodal solutions and we develop new concentration-compactness lemmas for sign-changing Palais--Smale sequences. The nonlinear Schr\"odinger equation, which is the nonlocal counterpart of the Choquard equation, does not have such solutions.Comment: 23 pages, revised version with additional details and symmetry properties of odd solution

    Soliton dynamics of NLS with singular potentials

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    We investigate the validity of a soliton dynamics behavior in the semi-relativistic limit for the nonlinear Schr\"odinger equation in RN,N3\R^{N}, N\ge 3, in presence of a singular external potential.Comment: 23 page

    On Yamabe type problems on Riemannian manifolds with boundary

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    Let (M,g)(M,g) be a nn-dimensional compact Riemannian manifold with boundary. We consider the Yamabe type problem \begin{equation} \left\{ \begin{array}{ll} -\Delta_{g}u+au=0 & \text{ on }M \\ \partial_\nu u+\frac{n-2}{2}bu= u^{{n\over n-2}\pm\varepsilon} & \text{ on }\partial M \end{array}\right. \end{equation} where aC1(M),a\in C^1(M), bC1(M)b\in C^1(\partial M), ν\nu is the outward pointing unit normal to M\partial M and ε\varepsilon is a small positive parameter. We build solutions which blow-up at a point of the boundary as ε\varepsilon goes to zero. The blowing-up behavior is ruled by the function bHg,b-H_g , where HgH_g is the boundary mean curvature

    Soliton dynamics for the generalized Choquard equation

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    We investigate the soliton dynamics for a class of nonlinear Schr\"odinger equations with a non-local nonlinear term. In particular, we consider what we call {\em generalized Choquard equation} where the nonlinear term is (xθNup)up2u(|x|^{\theta-N} * |u|^p)|u|^{p-2}u. This problem is particularly interesting because the ground state solutions are not known to be unique or non-degenerate.Comment: 16 page
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