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Decay of Correlations in 1D Lattice Systems of Continuous Spins and Long-Range Interaction

机译:自旋和远距离相互作用的一维晶格系统的相关性衰减

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We consider a one-dimensional lattice system of unbounded and continuous spins. The Hamiltonian consists of a perturbed strictly-convex single-site potential and a product term with longe-range interaction. We show that if the interactions have an algebraic decay of order 2+α,α > 0, then the correlations also decay algebraically of order 2+α for some α > α > 0. For the argument we generalize a method due to Zegarlinski from finite-range to infinite-range interaction to get a preliminary decay of correlations, which is improved to the correct order by a recursive scheme based on Lebowitz inequalities. Because the decay of correlations yields the uniqueness of the Gibbs measure, the main result of this article yields that the one-phase region of a continuous spin system is at least as large as for the Isingmodel. This shows that there is no-phase transition in one-dimensional systems of unbounded and continuous spins as long as the interaction decays algebraically of order 2 + α, α > 0.
机译:我们考虑无界和连续自旋的一维晶格系统。哈密​​顿量由摄动的严格凸的单点势和具有长程相互作用的乘积项组成。我们证明,如果相互作用具有2 +α,α> 0阶的代数衰减,那么对于某些α>α> 0,相关性也代数2 +α代数衰减。对于自变量,我们归纳了Zegarlinski提出的方法有限范围到无限范围的相互作用以获得相关性的初步衰减,通过基于Lebowitz不等式的递归方案将其改进为正确的阶数。由于相关性的衰减产生了吉布斯测度的唯一性,因此本文的主要结果是,连续自旋系统的单相区域至少与Isingmodel一样大。这表明,只要相互作用的代数以2 +α,α> 0的阶数衰减,在无界和连续自旋的一维系统中就没有相变。

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