Global well-posedness and stability of constant equilibria in parabolic–elliptic chemotaxis systems without gradient sensing
Global well-posedness and stability of constant equilibria in parabolic–elliptic chemotaxis
systems without gradient sensing Page 1 Nonlinearity PAPER Global well-posedness and …
systems without gradient sensing Page 1 Nonlinearity PAPER Global well-posedness and …
Spikes in two coupled nonlinear Schrödinger equations
TC Lin, J Wei - Annales de l'Institut Henri Poincaré C, Analyse non …, 2005 - Elsevier
Here we study the interaction and the configuration of spikes in a double condensate by
analyzing least energy solutions of two coupled nonlinear Schrödinger equations which …
analyzing least energy solutions of two coupled nonlinear Schrödinger equations which …
On Bound States Concentrating on Spheres for the Maxwell--Schrödinger Equation
T D'Aprile, J Wei - SIAM journal on mathematical analysis, 2005 - SIAM
We study the semiclassical limit for the following system of Maxwell--Schrödinger equations: -
ℏ^22mΔv+v+ωϕv-γv^p=0,\;\;-Δϕ=4πωv^2, where ℏ, m, ω, γ>0, v, ϕ:R^3→R, 1<p<117. This …
ℏ^22mΔv+v+ωϕv-γv^p=0,\;\;-Δϕ=4πωv^2, where ℏ, m, ω, γ>0, v, ϕ:R^3→R, 1<p<117. This …
Boundary concentration phenomena for a singularly perturbed elliptic problem
A Malchiodi, M Montenegro - … : A Journal Issued by the Courant …, 2002 - Wiley Online Library
We exhibit new concentration phenomena for the equation− ε2 Δu+ u= up in a smooth
bounded domain Ω⊆ ℝ2 and with Neumann boundary conditions. The exponent p is …
bounded domain Ω⊆ ℝ2 and with Neumann boundary conditions. The exponent p is …
On the number of interior peak solutions for a singularly perturbed Neumann problem
We consider the following singularly perturbed Neumann problem: ϵ^ 2 Δ u-u+ f (u)=
0\enspace\rm in\Omega,\quad\it u>\rm 0\enspace\rm in\Omega, ∂\it u ∂ ν= 0\enspace\rm …
0\enspace\rm in\Omega,\quad\it u>\rm 0\enspace\rm in\Omega, ∂\it u ∂ ν= 0\enspace\rm …
Singularly perturbed elliptic equations with symmetry: existence of solutions concentrating on spheres, Part II
A Ambrosetti, A Malchiodi, WM Ni - Indiana University mathematics journal, 2004 - JSTOR
We study the equation− ε2Δu+ V (| x|) u= up, with ε> 0 and p> 1, in balls or annuli of ℝn,
under Neumann or Dirichlet boundary conditions. As ε tends to zero we prove existence of …
under Neumann or Dirichlet boundary conditions. As ε tends to zero we prove existence of …
Multidimensional boundary layers for a singularly perturbed Neumann problem
A Malchiodi, M Montenegro - 2004 - projecteuclid.org
We continue the study of 34, proving concentration phenomena for the equation− ε 2 Δ u+
u= up in a smooth bounded domain Ω⊆ R^n and with Neumann boundary conditions. The …
u= up in a smooth bounded domain Ω⊆ R^n and with Neumann boundary conditions. The …
Qualitative properties of solutions to elliptic problems
WM Ni - Handbook of differential equations: stationary partial …, 2004 - Elsevier
Qualitative properties of solutions to elliptic equations can be interpreted in an extremely
broad sense to include virtually every property of solutions. In this chapter, however, I shall …
broad sense to include virtually every property of solutions. In this chapter, however, I shall …
Standing waves in the Maxwell-Schrödinger equation and an optimal configuration problem
T D'Aprile, J Wei - Calculus of Variations and Partial Differential …, 2006 - Springer
We study the following system of Maxwell-Schrödinger equations Δ uu-δ u\psi+ f (u)=
0,\quad Δ ψ+ u^ 2= 0 in\mathbb R^ N, u,\; ψ> 0,\quad u,\; ψ → 0\mbox as ‖ x| →+ ∞, where …
0,\quad Δ ψ+ u^ 2= 0 in\mathbb R^ N, u,\; ψ> 0,\quad u,\; ψ → 0\mbox as ‖ x| →+ ∞, where …
Multiple radial positive solutions of semilinear elliptic problems with Neumann boundary conditions
D Bonheure, C Grumiau, C Troestler - Nonlinear Analysis: Theory, Methods …, 2016 - Elsevier
Let BR be a ball of radius R in R N. We analyze the positive solutions to the problem {− Δ u+
u=| u| p− 2 u, in BR,∂ ν u= 0, on∂ BR, that branch out from the constant solution u= 1 as p …
u=| u| p− 2 u, in BR,∂ ν u= 0, on∂ BR, that branch out from the constant solution u= 1 as p …