A review on singularly perturbed differential equations with turning points and interior layers

KK Sharma, P Rai, KC Patidar - Applied Mathematics and computation, 2013 - Elsevier
Singular perturbation problems with turning points arise as mathematical models for various
physical phenomena. The problem with interior turning point represent one-dimensional …

The ground state of a Gross–Pitaevskii energy with general potential in the Thomas–Fermi limit

G Karali, C Sourdis - Archive for Rational Mechanics and Analysis, 2015 - Springer
We study the ground state which minimizes a Gross–Pitaevskii energy with general non-
radial trapping potential, under the unit mass constraint, in the Thomas–Fermi limit where a …

Clustering of boundary interfaces for an inhomogeneous Allen–Cahn equation on a smooth bounded domain

L Duan, S Wei, J Yang - Calculus of Variations and Partial Differential …, 2021 - Springer
We consider the inhomogeneous Allen–Cahn equation ϵ^ 2 Δ u\,+\, V (y)(1-u^ 2)\, u\,=\,
0\quad in\Omega,\qquad ∂ u ∂ ν\,=\, 0\quad on\partial Ω, ϵ 2 Δ u+ V (y)(1-u 2) u= 0 in Ω,∂ …

CLUSTERED INTERIOR PHASE TRANSITION LAYERS FOR AN INHOMOGENEOUS ALLEN-CAHN EQUATION IN HIGHER DIMENSIONAL DOMAINS.

J Yang, X Yang - Communications on Pure & Applied …, 2013 - search.ebscohost.com
For a singularly perturbed equation of inhomogeneous Allen-Cahn type with positive
potential function in high dimensional general domain, we prove the existence of solutions …

[HTML][HTML] Phase transition layers with boundary intersection for an inhomogeneous Allen–Cahn equation

XQ Fan, B Xu, J Yang - Journal of Differential Equations, 2019 - Elsevier
We consider the nonlinear problem of inhomogeneous Allen–Cahn equation ϵ 2 Δ u+ V (y)
u (1− u 2)= 0 in Ω,∂ u∂ ν= 0 on∂ Ω, where Ω is a bounded domain in R 2 with smooth …

Coexistence of two interfaces for an anisotropic Fife-Greenlee equation

W Liang, J Yang - Discrete and Continuous Dynamical Systems, 2024 - aimsciences.org
We consider the nonlinear problem of anisotropic Fife-Greenlee equation ε2div (∇ a (y)
u)+(u− P (y))(1− u2)= 0 inΩ,∇ a (y) u· ν= 0 on∂ Ω, where Ω is a bounded domain in R2 with …

Existence, local uniqueness and asymptotic approximation of spike solutions to singularly perturbed elliptic problems

O Omel'chenko, L Recke - 2011 - oa.tib.eu
This paper concerns general singularly perturbed second order semilinear elliptic equations
on bounded domains $ Omega subset R^ n $ with nonlinear natural boundary conditions …

Radial and bifurcating non-radial solutions for a singular perturbation problem in the case of exchange of stabilities

G Karali, C Sourdis - Annales de l'Institut Henri Poincaré C, Analyse non …, 2012 - Elsevier
We consider the singular perturbation problem− ε2Δu+ (u− a (| x|))(u− b (| x|))= 0 in the unit
ball of RN, N⩾ 1, under Neumann boundary conditions. The assumption that a (r)− b (r) …

Toda system and cluster phase transition layers in an inhomogeneous phase transition model

J Wei, J Yang - Asymptotic Analysis, 2010 - content.iospress.com
1− u 2)= 0 in Ω,∂ u∂ ν= 0 on∂ Ω, where Ω is a bounded domain in R2 with smooth
boundary,− 1< a (y)< 1, ε is a small parameter, ν denotes the outward normal of∂ Ω …

The Gel'fand Problem on Expanding Tubular Domains in : Existence and the Morse Index of Solutions

M Ghergu, Y Miyamoto - The Journal of Geometric Analysis, 2025 - Springer
We discuss the existence and the Morse index of solutions to the problem Δ U+ λ e U= 0 in Ω
R, U= 0 on∂ Ω R, where Ω R is a tubular domain in the plane with fixed width. We obtain the …