Results 101 to 110 of about 1,216,221 (148)
Odd symmetry of least energy nodal solutions for the Choquard equation
We consider the Choquard equation (also known as stationary Hartree equation or Schrödinger–Newton equation) −Δu+u=(Iα⋆|u|p)|u|p−2u.
Ruiz, David +3 more
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Solutions to discrete nonlinear Kirchhoff–Choquard equations
18 ...
openaire +2 more sources
Multiple nodal solutions of nonlinear Choquard equations
In this article, we consider the existence of multiple nodal solutions of the nonlinear Choquard equation $$\displaylines{ -\Delta u+u=(|x|^{-1}\ast|u|^p)|u|^{p-2}u \quad \text{in }\mathbb{R}^3,\cr u\in H^1(\mathbb{R}^3), }$$ where $p\in (5/2,5 ...
Zhihua Huang, Jianfu Yang, Weilin Yu
doaj
Normalized ground state solutions for a mass supercritical Choquard equation
This paper is concerned with the existence of normalized ground state solutions for a class of nonlinear Choquard equations with mass supercritical growth.
Kaizhen Yang, Xianyong Yang
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Multiple solutions for nonhomogeneous Choquard equations
In this article, we consider the multiple solutions for the nonhomogeneous Choquard equations $$ - \Delta u +u=\Big(\frac{1}{|x|^{\alpha}}\ast |u|^{p}\Big)|u|^{p-2}u+h(x), \quad x\in \mathbb{R}^N, $$ and $$ - \Delta u=\Big(\frac{1}{|x|^{\alpha ...
Lixia Wang
doaj
Normalized ground states for a kind of Choquard–Kirchhoff equations with critical nonlinearities
In this paper, we consider the existence of a normalized ground-state solution for the Choquard–Kirchhoff equation: { − ( a + b ∫ R 3 | ∇ u | 2 d x ) Δ u = λ u + μ ( I α ∗ | u | p ) | u | p − 2 u + ω | u | 4 u , in R 3 , u > 0 , ∫ R 3 | u | 2 = m 2 , in ...
Jiayi Fei, Qiongfen Zhang
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Ground state solutions for Choquard type equations with a singular potential
This article concerns the Choquard type equation $$ -\Delta u+V(x)u=\Big(\int_{\mathbb{R}^N}\frac{|u(y)|^p}{|x-y|^{N-\alpha}}dy\Big) |u|^{p-2}u,\quad x\in \mathbb{R}^N, $$ where $N\geq3$, $\alpha\in ((N-4)_+,N)$, $2\leq p
Tao Wang
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Multiple concentrating solutions for a fractional (p, q)-Choquard equation
We focus on the following fractional (p, q)-Choquard problem: (−Δ)psu+(−Δ)qsu+V(εx)(|u|p−2u+|u|q−2u)=1|x|μ*F(u)f(u) in RN,u∈Ws,p(RN)∩Ws,q(RN),u>0 in RN, $\begin{cases}{\left(-{\Delta}\right)}_{p}^{s}u+{\left(-{\Delta}\right)}_{q}^{s}u+V\left(\varepsilon ...
Ambrosio Vincenzo
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Ground state solution for Schrödinger-Choquard equation: doubly critical case
In this paper, we investigate the following Schrödinger-Choquard equation: − Δ u + u = ( I α ∗ | u | 2 α ♯ ) | u | 2 α ♯ − 2 u + | u | q − 2 u + | u | r − 2 u , x ∈ R N , $$ -\Delta u+u = (I_{\alpha }*|u|^{2_{\alpha }^{\sharp }})|u|^{2_{\alpha }^{ \sharp
Yusheng Shen, Zhiwei Zou, You Gao
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On nonhomogeneous Choquard equation with Hardy–Littlewood–Sobolev critical nonlinearity
In this paper, we investigate the existence of nontrivial solutions to the following critical nonhomogeneous Choquard equation: { − Δ u = λ u + ∫ Ω ( | u ( y ) | 2 α ∗ | x − y | α d y ) | u | 2 α ∗ − 2 u + f ( x ) i n Ω , u ∈ H 0 1 ( Ω ) , $$ \left ...
Rachid Echarghaoui +2 more
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