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高斯态层析成像中的对数对数困境

The log log jam in Gaussian state tomography

Sitan Chen, Weiyuan Gong, Qi Ye, Zhihan Zhang

arXiv 2607.12983首次发表:更新:

AI 中文总结

研究连续变量系统中高斯态层析成像样本复杂度问题,证明高斯测量协议有\(\log \log E\)依赖,给出自适应与能量依赖权衡协议,还表明非高斯测量及特定简单协议可降低样本复杂度,阐明能量作用及相关相互作用。

AI 中文摘要

与有限维情况不同,连续变量系统中的量子信息有一特殊性质:在不施加物理约束时,态层析成像的样本复杂度可能无界。值得注意的是,对于学习高斯态的现有最先进协议(其具有有限维描述)也是如此,已知最佳速率与\(\log \log E\)成比例,其中\(E\)是系统能量。我们证明这并非现有分析的人为产物,而是所用测量的基本限制。我们表明:(1)任何使用高斯测量的协议,即使是纠缠或自适应选择的协议,都必然有\(\log \log E\)的依赖关系,这回答了先前许多工作提出的一个开放性问题。(2)在自适应轮数和能量依赖之间存在平滑权衡,我们给出了一个实现此插值速率的匹配协议。(3)使用高度纠缠的非高斯测量,可以用\(O(n^2 / \epsilon^2)\)个样本学习\(n\)模纯高斯态,与\(E\)无关,这回答了Chen等人提出的一个开放性问题。(4)基于Holevo和Helstrom的单拷贝规范相位POVM的简单协议可以用\(O(1/\epsilon^2)\)个样本学习单模纯高斯态,同样与\(E\)无关。我们的结果阐明了能量在玻色子态层析成像中的作用,并为量子学习中自适应、纠缠和神奇性之间有趣的相互作用提供了新的见解。

英文摘要

Unlike in finite dimensions, quantum information in continuous-variable systems has the peculiar feature that without imposing physical constraints, the sample complexity of state tomography can be unbounded. Remarkably, this is even the case for state-of-the-art protocols for learning Gaussian states, which have finite-dimensional descriptions: the best known rates scale with $\log \log E$, where $E$ is the energy of the system. We prove this is not an artifact of existing analyses, but a fundamental limitation of the measurements used. We show: (1) Any protocol that uses Gaussian measurements, even entangled or adaptively chosen ones, must incur a $\log \log E$ dependence. This answers an open question posed by a number of previous works. (2) There is a smooth tradeoff between the number of rounds of adaptivity and the energy dependence, and we give a matching protocol achieving this interpolated rate. (3) With highly entangled, non-Gaussian measurements, one can learn $n$-mode pure Gaussian states with $O(n^2 / ε^2)$ samples, independent of $E$. This answers an open question posed by Chen et al. (4) A simple protocol based on the single-copy canonical phase POVM of Holevo and Helstrom learns single-mode pure Gaussian states with $O(1/ε^2)$ samples, again independent of $E$. Our results clarify the role of energy in bosonic state tomography and shed new light on the intriguing interplay between adaptivity, entanglement, and magic in quantum learning.

Comments70 pages, 2 figures, comments welcome

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