Existence and concentration of solution for a class of fractional Hamiltonian systems with subquadratic potential

preprint2015arXivOpen access

Abstract

This article study the fractional Hamiltonian systems \begin{eqnarray}\label{00} {_{t}}D_{\infty}^α({_{-\infty}}D_{t}^αu) + λL(t)u = \nabla W(t, u), \;\;t\in \mathbb{R}, \end{eqnarray} where α∈(1/2,1)α\in (1/2, 1), λ>0λ>0 is a parameter, L∈C(R,Rn×n)L\in C(\mathbb{R}, \mathbb{R}^{n\times n}) and W∈C1(R×Rn,R)W \in C^{1}(\mathbb{R} \times \mathbb{R}^n, \mathbb{R}). Unlike most other papers on this problem, we require that L(t)L(t) is a positive semi-definite symmetric matrix for all t∈Rt\in \mathbb{R}, that is, L(t)≡0L(t) \equiv 0 is allowed to occur in some finite interval I\mathbb{I} of R\mathbb{R}. Under some mild assumptions on WW, we establish the existence of nontrivial weak solution, which vanish on R∖I\mathbb{R} \setminus \mathbb{I} as λ→∞,λ\to \infty, and converge to u~\tilde{u} in Hα(R)H^α(\mathbb{R}); here u~∈E0α\tilde{u} \in E_{0}^α is nontrivial weak solution of the Dirichlet BVP for fractional Hamiltonian systems on the finite interval I\mathbb{I}.

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