Generalized hydrodynamics for the volterra lattice: ballistic and non-ballistic behavior of correlation functions

IF 2 3区 物理与天体物理 Q2 PHYSICS, MATHEMATICAL
Guido Mazzuca
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引用次数: 0

Abstract

In recent years, a lot of effort has been put in describing the hydrodynamic behavior of integrable systems. In this paper, we describe such picture for the Volterra lattice. Specifically, we are able to explicitly compute the susceptibility matrix and the current-field correlation matrix in terms of the density of states of the Volterra lattice endowed with a Generalized Gibbs ensemble. Furthermore, we apply the theory of linear Generalized Hydrodynamics (GHDs) to describe the Euler scale behavior of the correlation functions. We anticipate that the solution to the GHDs equations develops shocks at ; so this linear approximation does not fully describe the behavior of correlation functions. Intrigued by this fact, we performed several numerical investigations which show that, exactly when the solution to the hydrodynamic equations develops shock, the correlation functions show an highly oscillatory behavior. In view of this empirical observation, we believe that at this point ξ0 the diffusive contribution are not sub-leading corrections to the ballistic transport, but they are of the same order.
伏特拉晶格的广义流体力学:相关函数的弹道和非弹道行为
近年来,人们在描述可积分系统的流体力学行为方面投入了大量精力。在本文中,我们描述了 Volterra 晶格的这种情况。具体地说,我们能够根据具有广义吉布斯集合的 Volterra 晶格的状态密度,明确计算易感性矩阵和电流场相关矩阵。此外,我们还应用线性广义流体力学(GHD)理论来描述相关函数的欧拉尺度行为。我们预计,GHDs方程的解在;处会产生冲击,因此这种线性近似并不能完全描述相关函数的行为。出于对这一事实的好奇,我们进行了一些数值研究,结果表明,正是在流体力学方程的解产生冲击时,相关函数才会表现出高度振荡的行为。鉴于这一经验观察结果,我们认为在 ξ0 点,扩散贡献不是对弹道传输的次领先修正,而是具有相同的阶数。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
CiteScore
4.10
自引率
14.30%
发文量
542
审稿时长
1.9 months
期刊介绍: Publishing 50 issues a year, Journal of Physics A: Mathematical and Theoretical is a major journal of theoretical physics reporting research on the mathematical structures that describe fundamental processes of the physical world and on the analytical, computational and numerical methods for exploring these structures.
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