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Dynamics of the Heisenberg model and a theorem on stability

机译:海森堡模型的动力学和稳定性定理

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We consider the general discrete classical Heisenberg model (HM) with z axis anisotropy and external magnetic field and show that its phase space is foliated into a family of invariant manifolds (the leaves) diffeomorphic to (S~2)λ, where λ is the number of spins. We also show that the flow on each leaf S is Hamiltonian. Subsequently, we focus on the isotropic HM in the absence of external field. We discuss the rotational symmetry of the model and further analyze its phase space structure. We prove that the manifold F of longitudinal fixed points intersects each leaf S orthogonally. For a real local flow with a continuous symmetry, we show that the Lyapunov stability of invariant sets on an invariant subspace can be extended to the whole phase space. This general theorem is the main result of the article. We use it to show that, in the case of the isotropic HM, the ferromagnetic state and the antiferromagnetic state with non-zero total spin are both stable fixed points. The theorem does not apply at total spin zero, and indeed the AF state on an equal-spins leaf is found to be unstable.
机译:我们考虑了具有z轴各向异性和外部磁场的一般离散经典Heisenberg模型(HM),并证明了其相空间叶型化为(S〜2)λ变质的不变流形(叶)族,其中λ是转数。我们还表明,每个叶子S上的流动都是哈密顿量。随后,我们在没有外部场的情况下关注各向同性HM。我们讨论了模型的旋转对称性,并进一步分析了其相空间结构。我们证明纵向固定点的流形F与每个叶子S正交。对于具有连续对称性的真实局部流,我们证明不变子空间上的不变集的Lyapunov稳定性可以扩展到整个相空间。这个一般定理是本文的主要结果。我们用它来证明,在各向同性HM的情况下,总自旋非零的铁磁状态和反铁磁状态都是稳定的固定点。该定理不适用于总自旋为零,并且确实发现等旋转叶片上的AF状态不稳定。

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