## Abstract Using a general symmetry approach we establish transformations between different non‐linear space–time dependent evolution equations of Schrödinger type and their respective solutions. As a special case we study the transformation of the standard non‐linear Schrödinger equation (NLS)‐eq
Ground state solutions of non-linear singular Schrödinger equations with lack of compactness
✍ Scribed by Mihai Mihǎilescu; Vicenţiu Rǎdulescu
- Publisher
- John Wiley and Sons
- Year
- 2003
- Tongue
- English
- Weight
- 104 KB
- Volume
- 26
- Category
- Article
- ISSN
- 0170-4214
- DOI
- 10.1002/mma.403
No coin nor oath required. For personal study only.
✦ Synopsis
Abstract
We study a class of time‐independent non‐linear Schrödinger‐type equations on the whole space with a repulsive singular potential in the divergence operator and we establish the existence of non‐trivial standing wave solutions for this problem in an appropriate weighted Sobolev space. Such equations have been derived as models of several physical phenomena. Our proofs rely essentially on critical point theory tools combined with the Caffarelli–Kohn–Nirenberg inequality. Copyright © 2003 John Wiley & Sons, Ltd.
📜 SIMILAR VOLUMES
An extension to the theory of Schrodinger equations has been made ẅhich enables the derivation of eigenvalues from a consideration of a very small part of geometric space. The concomitant unwanted continuum effects have been removed. The theory enables very convergent or ''superconvergent'' calculat
In this article exact solutions of a two-electron Schrödinger equation for the Coulomb potential were extended to the Fues-Kratzer-type potential: ( Ẑ( )/r) + ( Â/r 2 ). The wave function (r, ) is expanded into generalized Laguerre polynomials and hyperspherical harmonics. An analytical expression o
## Abstract We consider the blowup of solutions of the initial boundary value problem for a class of non‐linear evolution equations with non‐linear damping and source terms. By using the energy compensation method, we prove that when __p__>max{__m__, __α__}, where __m__, __α__ and __p__ are non‐neg