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Condensed Matter > Disordered Systems and Neural Networks

arXiv:2408.02016 (cond-mat)
[Submitted on 4 Aug 2024 (v1) , last revised 18 Aug 2025 (this version, v2)]

Title: Dynamics of many-body localized systems: logarithmic lightcones and $\log \, t$-law of $α$-Rényi entropies

Title: 多体局域化系统的动力学:对数光锥和$\log \, t$-定律的$α$-Rényi 熵

Authors:Daniele Toniolo, Sougato Bose
Abstract: In the context of the Many-Body-Localization phenomenology we consider arbitrarily large one-dimensional local spin systems, the XXZ model with random magnetic field is a prototypical example. Without assuming the existence of exponentially localized integrals of motion (LIOM), but assuming instead that the system's dynamics gives rise to a Lieb-Robinson bound (L-R) with a logarithmic lightcone, we rigorously evaluate the dynamical generation, starting from a generic product state, of $ \alpha$-R\'enyi entropies, with $ \alpha $ close to one, obtaining a $\log \, t$-law, that denotes a slow spread of entanglement. This is in sharp contrast with Anderson localized phases that show no dynamically generated entanglement. To prove this result we apply a general theory recently developed by us in arXiv:2408.00743 that quantitatively relates the L-R bounds of a local Hamiltonian with the dynamical generation of entanglement. Assuming instead the existence of LIOM we provide new independent proofs of the known facts that the L-R bound of the system's dynamics has a logarithmic light cone and show that the dynamical generation of the von Neumann entropy has for large times a $ \log \, t$-shape. L-R bounds, that quantify the dynamical spreading of local operators, may be easier to measure in experiments in comparison to global quantities such as entanglement.
Abstract: 在多体局域化现象学的背景下,我们考虑任意大的一维局部自旋系统,具有随机磁场的XXZ模型是一个典型的例子。 不假设存在指数局域化的守恒量(LIOM),而是假设系统的动力学导致了具有对数光锥的Lieb-Robinson界限(L-R),我们严格评估了从一般乘积态开始的动力学生成的$ \alpha$-黎曼熵,其中$ \alpha $接近于一,得到一个$\log \, t$定律,表示纠缠的缓慢传播。 这与展示没有动态生成纠缠的安德森局域相位形成鲜明对比。 为了证明这个结果,我们应用了我们最近在arXiv:2408.00743中开发的一般理论,该理论定量地将局部哈密顿量的L-R界限与纠缠的动力学生成联系起来。 假设LIOM的存在,我们提供了新的独立证明,已知事实是系统的L-R界限具有对数光锥,并表明冯·诺依曼熵的动力学生成在长时间下具有$ \log \, t$形状。 量化局部算符动力学扩展的L-R界限,在实验中可能比纠缠等全局量更容易测量。
Comments: v2: improved introduction, simplified proof of theorem 1, added references
Subjects: Disordered Systems and Neural Networks (cond-mat.dis-nn) ; Mesoscale and Nanoscale Physics (cond-mat.mes-hall); Mathematical Physics (math-ph); Quantum Physics (quant-ph)
Cite as: arXiv:2408.02016 [cond-mat.dis-nn]
  (or arXiv:2408.02016v2 [cond-mat.dis-nn] for this version)
  https://doi.org/10.48550/arXiv.2408.02016
arXiv-issued DOI via DataCite

Submission history

From: Daniele Toniolo [view email]
[v1] Sun, 4 Aug 2024 12:53:55 UTC (26 KB)
[v2] Mon, 18 Aug 2025 01:17:46 UTC (31 KB)
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