测量诱导量子动力学的无选择后学习

Max McGinley
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引用次数: 0

摘要

我们探讨了如何根据经验推断由涉及测量的动力学产生的量子态的属性。我们的重点是多体环境,在这种环境中,测量的数量非常多,基于后选择的粗暴方法因其指数级的样本复杂性而难以操作。我们引入了一种通用方案,可用于使用可扩展的实验重复次数来推断测量后状态集合的任何属性(如平均纠缠熵或框架势)。我们首先确定了一类可直接从实验数据中提取的 "可估算属性"。然后,基于对此类量的经验观察,我们展示了如何通过经典的后处理间接推断出任何特定的非可估量相关量的信息。我们的方法基于优化任务,即在确保与观测结果一致的前提下,询问所需量可能取的最小值和最大值是多少。然后,这个量的真实值必须位于这些极值之间的可行范围内,从而产生双侧边界。通过对设备进行经典模拟,确定应测量的可估算属性,可以获得较窄的可行范围。即使在模拟不准确的情况下,也能了解量子设备上实现的给定数量的真实值。作为直接应用,我们展示了我们的方法可用于验证实验中量子态设计的出现。我们确定了一些基本障碍,这些障碍在某些情况下会阻止推断出给定量的尖锐知识,并讨论了在经典模拟对计算要求太高而不可行的情况下可以学到什么。特别是,我们证明了任何无法进行经典模拟的观察者都无法将输出状态与从最大无结构集合中采样的状态区分开来。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Postselection-Free Learning of Measurement-Induced Quantum Dynamics

Postselection-Free Learning of Measurement-Induced Quantum Dynamics
We address how one can empirically infer properties of quantum states generated by dynamics involving measurements. Our focus is on many-body settings where the number of measurements is extensive, making brute-force approaches based on postselection intractable due to their exponential sample complexity. We introduce a general-purpose scheme that can be used to infer any property of the postmeasurement ensemble of states (e.g., the average entanglement entropy, or frame potential) using a scalable number of experimental repetitions. We first identify a general class of “estimable properties” that can be directly extracted from experimental data. Then, based on empirical observations of such quantities, we show how one can indirectly infer information about any particular given nonestimable quantity of interest through classical postprocessing. Our approach is based on an optimization task, where one asks what are the minimum and maximum values that the desired quantity could possibly take, while ensuring consistency with observations. The true value of this quantity must then lie within a feasible range between these extrema, resulting in two-sided bounds. Narrow feasible ranges can be obtained by using a classical simulation of the device to determine which estimable properties one should measure. Even in cases where this simulation is inaccurate, unambiguous information about the true value of a given quantity realized on the quantum device can be learned. As an immediate application, we show that our method can be used to verify the emergence of quantum state designs in experiments. We identify some fundamental obstructions that in some cases prevent sharp knowledge of a given quantity from being inferred, and discuss what can be learned in cases where classical simulation is too computationally demanding to be feasible. In particular, we prove that any observer who cannot perform a classical simulation cannot distinguish the output states from those sampled from a maximally structureless ensemble.
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