错误:搜索内容不能为空,请输入英文关键词
错误:关键词超出字数限制,请精简
高级检索

Classification, non-degeneracy and existence of solutions to nonlinear Choquard equations

  • Zhihua Huang,
  • Chao Liu

摘要

In this paper, we first study the classification problem of positive solutions to the nonlocal Choquard equation \(\begin{aligned} (-\Delta )^{\alpha }u=\left( \textrm{I}_{\beta }*\left| u\right| ^{p}\right) \left| u\right| ^{p-2}u, \qquad u\in {\mathcal {D}}^{\alpha ,2}\left( {\mathbb {R}}^N\right) \cap L^{\frac{2Np}{N+\beta }}\left( {\mathbb {R}}^N\right) , \end{aligned}\) ( - Δ ) α u = I β u p u p - 2 u , u D α , 2 R N L 2 N p N + β R N , where \(\alpha \in \left( 0,\frac{N}{2}\right) \) α 0 , N 2 with \(N\ge 1\) N 1 , \(\textrm{I}_{\beta }(x)\) I β ( x ) is the standard Riesz potential with \(\beta \in \left( 0,N\right) \) β 0 , N if \(N\le 4\alpha \) N 4 α , or \(\beta \in \left[ N-4\alpha ,N\right) \) β N - 4 α , N if \(N>4\alpha \) N > 4 α , and \(p\in [2, 2^*_{\alpha ,\beta }]\) p [ 2 , 2 α , β ] with \(2^*_{\alpha ,\beta }:=\frac{N+\beta }{N-2\alpha }\) 2 α , β : = N + β N - 2 α which denotes the corresponding Hardy–Littlewood–Sobolev critical exponent. By applying the method of moving planes, we prove that the above Choquard equation has no positive solution in the subcritical case \(p\in [2, 2^*_{\alpha ,\beta })\) p [ 2 , 2 α , β ) , and any positive solution must be of the form \(\begin{aligned} U_{\lambda , x_0}(x)=C_{\alpha ,\beta ,N}\left( \frac{\lambda }{\lambda ^2 +\left| x-x^0\right| ^2}\right) ^{\frac{N-2\alpha }{2}} \end{aligned}\) U λ , x 0 ( x ) = C α , β , N λ λ 2 + x - x 0 2 N - 2 α 2 in the critical case \(p=2^*_{\alpha ,\beta }\) p = 2 α , β , where \(x^0\in {\mathbb {R}}^N\) x 0 R N , \(\lambda >0\) λ > 0 and the constant \(C_{\alpha ,\beta ,N}>0\) C α , β , N > 0 only depends on \(\alpha \) α , \(\beta \) β and N. Moreover, we prove that this solution \(U_{\lambda , x^0}(x)\) U λ , x 0 ( x ) is non-degenerate. Based on the non-degeneracy result, we study the existence of solutions to the following Choquard equation with potential: \(\begin{aligned} -\Delta u+V(\left| x\right| )u=\left( \textrm{I}_{\beta }*u^{2_{1, \beta }^*}\right) u^{2_{1,\beta }^*-1},\qquad u\in {\mathcal {D}}^{1,2}({\mathbb {R}}^N), \end{aligned}\) - Δ u + V ( x ) u = I β u 2 1 , β u 2 1 , β - 1 , u D 1 , 2 ( R N ) , where \(\beta \in [N-4,N-2)\) β [ N - 4 , N - 2 ) , \(N\ge 5\) N 5 , and \(V(\cdot )\) V ( · ) is a bounded non-negative function. We show that this Choquard equation possesses infinitely many non-radial solutions provided that \(r^{2}V(r)\) r 2 V ( r ) has an isolated local maximum point, or isolated local minimum point \(r_0>0\) r 0 > 0 satisfying \(V(r_0)>0\) V ( r 0 ) > 0 .