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arXiv 2004.11957cond-mat.stat-mechcond-mat.dis-nncond-mat.quant-gascond-mat.str-elquant-ph
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连续监测下的测量诱导量子临界性

Measurement-induced quantum criticality under continuous monitoring

Yohei Fuji, Yuto Ashida

摘要:

基于量子轨道方法,研究了连续位置测量下量子多体态中从体积纠缠到面积纠缠的相变。我们发现作为测量强度的函数的互信息的峰值结构的过渡的签名,如先前报道的随机酉电路与投影测量。在过渡点,纠缠熵规模代数和各种物理量规模代数,这意味着涌现共形临界,可积和不可积的一维相互作用哈密顿量;然而,这种转变已被认为是不存在的非相互作用制度在以前的一些研究。借助于我们模型中的$U(1)$对称性,测量诱导临界性表现出类似于Tomonaga-Luttinger液体理论的光谱特征。这些有趣的临界现象是唯一的稳态制度的条件动力学在单轨迹水平,并没有在无条件动力学遵守Lindblad主方程,其中系统最终与无特征的,无限温度的混合状态。我们还提出了一个可能的实验装置来测试预测的纠缠过渡的基础上的子系统的粒子数波动。这个量应该很容易通过量子气体显微镜的现有技术测量,并且在实践中比纠缠熵本身更容易获得。

英文摘要:

We investigate entanglement phase transitions from volume-law to area-law entanglement in a quantum many-body state under continuous position measurement on the basis of the quantum trajectory approach. We find the signatures of the transitions as peak structures in the mutual information as a function of measurement strength, as previously reported for random unitary circuits with projective measurements. At the transition points, the entanglement entropy scales logarithmically and various physical quantities scale algebraically, implying emergent conformal criticality, for both integrable and nonintegrable one-dimensional interacting Hamiltonians; however, such transitions have been argued to be absent in noninteracting regimes in some previous studies. With the aid of $U(1)$ symmetry in our model, the measurement-induced criticality exhibits a spectral signature resembling a Tomonaga-Luttinger liquid theory from symmetry-resolved entanglement. These intriguing critical phenomena are unique to steady-state regimes of the conditional dynamics at the single-trajectory level, and are absent in the unconditional dynamics obeying the Lindblad master equation, in which the system ends up with the featureless, infinite-temperature mixed state. We also propose a possible experimental setup to test the predicted entanglement transition based on the subsystem particle-number fluctuations. This quantity should readily be measured by the current techniques of quantum gas microscopy and is in practice easier to obtain than the entanglement entropy itself.

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