Nonintegrability of (2+1)-dimensional continuum isotropic Heisenberg spin system: Painlevé analysis
arXiv:nlin/0604017 · doi:10.1016/j.physleta.2006.03.074
Abstract
While many integrable spin systems are known to exist in (1+1) and (2+1) dimensions, the integrability property of the physically important (2+1) dimensional isotropic Heisenberg ferromagnetic spin system in the continuum limit has not been investigated in the literature. In this paper, we show through a careful singularity structure analysis of the underlying nonlinear evolution equation that the system admits logarithmic type singular manifolds and so is of non-Painlevé type and is expected to be nonintegrable.
arXiv comment11 pages. to be published in Phys. Lett. A (2006)
References in corpus (3)
- Motion of Curves and Surfaces and Nonlinear Evolution Equations in (2+1) Dimensions
- On the simplest (2+1) dimensional integrable spin systems and their equivalent nonlinear Schrödinger equations
- A (2+1) dimensional integrable spin model: Geometrical and gauge equivalent counterpart, solitons and localized coherent structures
Cited by in corpus (6)
- The Fascinating World of Landau-Lifshitz-Gilbert Equation: An Overview
- Integrable (2+1)-Dimensional Spin Models with Self-Consistent Potentials
- Darboux Transformation and Exact Solutions of the integrable Heisenberg ferromagnetic equation with self-consistent potentials
- Dynamic and Static Excitations of a Classical Discrete Anisotropic Heisenberg Ferromagnetic Spin Chain
- Integrable motion of two interacting curves, spin systems and the Manakov system
- Towers with skeletons for the (2+1)-dimensional continuous isotropic Heisenberg spin model