In this paper we study the shape of least-energy solutions to the quasilinear problem εmΔmu−um−1+f(u)=0 with homogeneous Neumann boundary condition. We use an intrinsic variation method to show that as ε→0+, the global maximum point Pε of least-energy solutions goes to a point on the boundary ∂Ω at the rate of o(ε) and this point on the boundary approaches to a point where the mean curvature of ∂Ω achieves its maximum. We also give a complete proof of exponential decay of least-energy solutions
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
AbstractWe consider the problem: −Δu + λu = un + 2)(n − 2, u > 0 in Ω, ∂u/∂v = 0 on ∂Ω, where Ω is a...
In this paper we study the shape of least-energy solutions to the quasilinear problem εmΔmu−um−1+f(u...
In this paper we study the shape of least-energy solutions to the quasilinear problem εmΔmu−um−1+f(u...
We continue our work (Y. Li, C. Zhao, Locating the peaks of least-energy solutions to a quasilinear ...
In this paper we study the shape of least-energy solutions to a singularly perturbed quasilinear pro...
In this paper we study the shape of least-energy solutions to a singularly perturbed quasilinear pro...
In this paper we study the shape of least-energy solutions to a singularly perturbed quasilinear pro...
Abstract: We study the shape of least-energy solutions to the quasilinear elliptic equation ∊mΔmu − ...
Abstract: We study the shape of least-energy solutions to the quasilinear elliptic equation ∊mΔmu − ...
AbstractWe consider a system of the form −ε2Δu+u=g(v),−ε2Δv+v=f(u) in Ω with Neumann boundary condit...
The paper is concerned with a system of the form −"2u+u = g(v), −"2v +v = f(u), in a smooth bounded ...
We consider the problem: -Δu + λu = un + 2)(n - 2, u > 0 in Ω , ∂u/∂v = 0 on ∂Ω, where Ω is a bou...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
AbstractWe consider the problem: −Δu + λu = un + 2)(n − 2, u > 0 in Ω, ∂u/∂v = 0 on ∂Ω, where Ω is a...
In this paper we study the shape of least-energy solutions to the quasilinear problem εmΔmu−um−1+f(u...
In this paper we study the shape of least-energy solutions to the quasilinear problem εmΔmu−um−1+f(u...
We continue our work (Y. Li, C. Zhao, Locating the peaks of least-energy solutions to a quasilinear ...
In this paper we study the shape of least-energy solutions to a singularly perturbed quasilinear pro...
In this paper we study the shape of least-energy solutions to a singularly perturbed quasilinear pro...
In this paper we study the shape of least-energy solutions to a singularly perturbed quasilinear pro...
Abstract: We study the shape of least-energy solutions to the quasilinear elliptic equation ∊mΔmu − ...
Abstract: We study the shape of least-energy solutions to the quasilinear elliptic equation ∊mΔmu − ...
AbstractWe consider a system of the form −ε2Δu+u=g(v),−ε2Δv+v=f(u) in Ω with Neumann boundary condit...
The paper is concerned with a system of the form −"2u+u = g(v), −"2v +v = f(u), in a smooth bounded ...
We consider the problem: -Δu + λu = un + 2)(n - 2, u > 0 in Ω , ∂u/∂v = 0 on ∂Ω, where Ω is a bou...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
We continue our work (Y. Li, C. Zhao in J Differ Equ 212:208–233, 2005) to study the structure of po...
AbstractWe consider the problem: −Δu + λu = un + 2)(n − 2, u > 0 in Ω, ∂u/∂v = 0 on ∂Ω, where Ω is a...