动态量子树上的测量诱导相变

IF 9.3 Q1 PHYSICS, APPLIED
Xiao-Min Feng, B. Skinner, A. Nahum
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引用次数: 10

摘要

受监测的多体系统大致分为两个动力学阶段,“纠缠”或“解纠缠”,由作为系统测量速率函数的转变分开。产生这种测量诱导的转变的分析理论是一个突出的挑战。最近的工作在树张量网络的背景下取得了进展,该网络可以与具有强制(事后选择)测量结果的所有量子电路动力学相关。然而,到目前为止,对于具有“真实”测量的自旋1/2自由度(量子位)的动力学,还没有精确的解,其结果概率是根据Born规则采样的。在这里,我们定义了量子位的动态过程,具有真实的测量结果,具有树状的时空交互图,可以将系统作为时间的函数进行折叠或扩展。前一种情况产生了一个精确可解的测量跃迁。我们利用树的递归结构,对这些过程进行了分析和数值研究。我们比较了“实际”测量和“强制”测量的情况。两种情况都显示出在测量强度的非平凡值处的跃迁,真实的测量情况显示出较小的纠缠阶段。两者在跃迁附近都表现出纠缠的指数标度,但它们在临界指数的值上不同。这两种情况之间的一个有趣的区别是,真实的测量情况位于两种不同类型的临界标度之间的边界。基于我们的结果,我们提出了一种通过扩展过程实验实现测量相变的协议。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Measurement-Induced Phase Transitions on Dynamical Quantum Trees

Measurement-Induced Phase Transitions on Dynamical Quantum Trees
Monitored many-body systems fall broadly into two dynamical phases, ``entangling'' or ``disentangling'', separated by a transition as a function of the rate at which measurements are made on the system. Producing an analytical theory of this measurement-induced transition is an outstanding challenge. Recent work made progress in the context of tree tensor networks, which can be related to all-to-all quantum circuit dynamics with forced (postselected) measurement outcomes. So far, however, there are no exact solutions for dynamics of spin-1/2 degrees of freedom (qubits) with ``real'' measurements, whose outcome probabilities are sampled according to the Born rule. Here we define dynamical processes for qubits, with real measurements, that have a tree-like spacetime interaction graph, either collapsing or expanding the system as a function of time. The former case yields an exactly solvable measurement transition. We explore these processes analytically and numerically, exploiting the recursive structure of the tree. We compare the case of ``real'' measurements with the case of ``forced'' measurements. Both cases show a transition at a nontrivial value of the measurement strength, with the real measurement case exhibiting a smaller entangling phase. Both exhibit exponential scaling of the entanglement near the transition, but they differ in the value of a critical exponent. An intriguing difference between the two cases is that the real measurement case lies at the boundary between two distinct types of critical scaling. On the basis of our results we propose a protocol for realizing a measurement phase transition experimentally via an expansion process.
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CiteScore
14.60
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0.00%
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