Standing waves with a critical frequency for nonlinear Choquard equations
In this paper, we study the nonlocal Choquard equation $$ -\varepsilon^2 \Delta u_\varepsilon + V u_\varepsilon= (I_\alpha * |u_\varepsilon|^p)|u_\varepsilon|^{p-2}u_\varepsilon $$ where $N\geq 1$, $I_\alpha$ is the Riesz potential of order $\alpha \in ...
Van Schaftingen, Jean, Xia, Jiankang
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A nontrivial solution for a nonautonomous Choquard equation with general nonlinearity
With the help of the monotonicity trick, a nonautonomous Choquard equations with general nonlinearity is studied and a nontrivial solution is obtained.
Ling Ding, Jiu Liu, Yan-Xiang Yuan
doaj +1 more source
Non-linear bi-harmonic Choquard equations
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
openaire +3 more sources
Existence of positive solutions to the nonlinear Choquard equation with competing potentials
This article concerns the existence of positive solutions of the nonlinear Choquard equation $$ -\Delta u+a(x)u=b(x)\Big(\frac{1}{|x|}*|u|^2\Big)u,\quad u\in H^{1}({\mathbb R}^3), $$ where the coefficients a and b are positive functions such that
Jun Wang, Mengmeng Qu, Lu Xiao
doaj
Global dynamics of the parabolic Choquard equation with asymptotically linear nonlinearity
This article investigates the global dynamics of the semilinear parabolic Choquard equation ∂ t u ( x , t ) − Δ u ( x , t ) + u ( x , t ) = ( I α ∗ | u ( ⋅ , t ) | p ) ( x ) | u ( x , t ) | p − 2 u ( x , t ) + f ( u ( x , t ) ) , ( x , t ) ∈ R N × ( 0 , ∞
Salah Boulaaras
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Can quantum systems succumb to their own (gravitational) attraction?
The gravitational interaction is generally considered to be too weak to be easily submitted to systematic experimental investigation in the quantum, microscopic, domain.
Colin, Samuel +2 more
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Nonlocal perturbations of the fractional Choquard equation
We study the ...
Singh Gurpreet
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On nonlinear fractional Choquard equation with indefinite potential and general nonlinearity
In this paper, we consider a class of fractional Choquard equations with indefinite potential ( − Δ ) α u + V ( x ) u = [ ∫ R N M ( ϵ y ) G ( u ) | x − y | μ d y ] M ( ϵ x ) g ( u ) , x ∈ R N , $$ (-\Delta )^{\alpha}u+V(x)u= \biggl[ \int _{{\mathbb{R ...
Fangfang Liao +3 more
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Semi-classical states for the Choquard equation [PDF]
28 pages, updated ...
Moroz, Vitaly, van Schaftingen, Jean
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Quantitative Properties on the Steady States to A Schr\"odinger-Poisson-Slater System [PDF]
A relatively complete picture on the steady states of the following Schr$\ddot{o}$dinger-Poisson-Slater (SPS) system \[ \begin{cases} -\Delta Q+Q=VQ-C_{S}Q^{2}, & Q>0\text{ in }\mathbb{R}^{3}\\ Q(x)\to0, & \mbox{as }x\to\infty,\\ -\Delta V=Q^{2}, & \text{
Xiang, Changlin
core

