arXivDaily arXiv每日学术速递 周一至周五更新
arXiv周末暂无论文更新,休息一下吧,周末愉快~~

纠缠测量对于混合费米子高斯态及真空附近玻色子高斯态的最优层析是必要的

Entangled measurements are necessary for optimal tomography of mixed fermionic Gaussian states and of bosonic Gaussian states near the vacuum

Ron Rubin

arXiv 2609.23189首次发表:更新:

发表机构

Rubin Anders Scientific, Inc.(鲁宾安德斯科学有限公司)

机构由 AI 辅助整理,请以论文原文为准。

AI 中文总结

本文证明混合费米子及真空附近玻色子高斯态的单副本层析下界为Ω(m³/ε²),与集体测量Θ(m²/ε²)分离,并给出双模纠缠优势的数值见证。

AI 中文摘要

我们证明,当测量每次仅作用于一个副本时,学习 $m$ 模上未知混合费米子高斯态至迹距离 $\epsilon$ 需要 $\Omega(m^3/\epsilon^2)$ 个副本,即使允许任意 POVM、新鲜辅助比特和经典自适应,但在副本之间没有量子内存。该下界适用于 $0<\epsilon\le1/3600$,并将此模型与已知的集体速率 $\Theta(m^2/\epsilon^2)$ 区分开来。它源于统一的单副本 Fisher 信息预算以及迹距离与高斯参数之间的维度无关比较。在算子范数至多 $1-c$ 的协方差矩阵上,我们证明了 Frobenius 到迹范数的连续性界,常数为 $[2c(2-c)]^{-1/2}$;matchgate 阴影随后达到 $O(m^3/(c\epsilon^2))$ 个副本。这也为热自由费米子态提供了显式误差证书。对于总平均光子数至多为一的一类混合被动玻色子高斯态,归约到有界块 qudit 层析给出了单副本下界 $\Omega(m^3/(\epsilon^2\sqrt{\log(m/\epsilon)}))$,而集体复杂度为 $\Theta(m^2/\epsilon^2)$。这些分离回答了 Chen 等人提出的混合态测量资源问题。一个双模例子具有最优两副本 Fisher 迹 $5$,而可分上限为 $4$。IBM 复制实验给出了预注册的见证下界 $4.12$,单侧 $95\\%$ 散粒噪声置信度;其解释假设了规定的制备和共同的测量通道,并且不约束制备系统误差。

英文摘要

We prove that learning an unknown mixed fermionic Gaussian state on $m$ modes to trace distance $ε$ requires $Ω(m^3/ε^2)$ copies when measurements act on one copy at a time, even with arbitrary POVMs, fresh ancillas and classical adaptivity, but without quantum memory between copies. The bound holds for $0<ε\le1/3600$ and separates this model from the known collective rate $Θ(m^2/ε^2)$. It follows from a uniform single-copy Fisher-information budget and a dimension-independent comparison between trace distance and Gaussian parameters. On covariance matrices of operator norm at most $1-c$, we prove a Frobenius-to-trace-norm continuity bound with constant $[2c(2-c)]^{-1/2}$; matchgate shadows then attain $O(m^3/(cε^2))$ copies. This also gives explicit error certificates for thermal free-fermion states. For a class of mixed passive bosonic Gaussian states with total mean photon number at most one, a reduction to bounded-block qudit tomography gives a single-copy lower bound $Ω(m^3/(ε^2\sqrt{\log(m/ε)}))$, versus collective complexity $Θ(m^2/ε^2)$. These separations answer the mixed-state measurement-resource question posed by Chen et al. A two-mode example has optimal two-copy Fisher trace $5$, versus the separable ceiling $4$. An IBM replication gave a pre-registered witness lower bound $4.12$ at one-sided $95\%$ shot-noise confidence; its interpretation assumes the prescribed preparations and a common measurement channel and does not bound preparation systematics.

Comments38 pages, 1 figure. Ancillary files: IBM pilot and replication data, circuits, and offline recount code

论文原文

arXiv 摘要页 · PDF 原文 · HTML 原文

↑