Online Shadow Tomography Matching the Classical Bounds
2026-07-31 • Data Structures and Algorithms
Data Structures and Algorithms
AI summaryⓘ
The authors study Online Shadow Tomography, a task where one must estimate measurements on an unknown quantum state repeatedly with limited copies. They improve prior methods by developing new algorithms that need fewer copies and better handle many measurements, matching the best known classical results. Their approach introduces a novel way to measure how quantum states get disturbed by measurements, using something called the quantum Efron–Stein decomposition. This work closes gaps in previous quantum measurement estimation techniques, even improving results for the simpler offline setting.
Quantum stateShadow TomographyAdaptive measurementsTrace estimationQuantum Efron–Stein decompositionQuantum measurement disturbanceAdaptive Data AnalysisQuantum algorithmsSample complexity
Authors
Sitan Chen, Ryan O'Donnell, Angelos Pelecanos, John Wright
Abstract
In \emph{Online Shadow Tomography}, we are given copies of an unknown $d$-dimensional quantum state $ρ$, an adversary (adaptively) proposes a sequence of bounded observables $A^{(1)},\ldots,A^{(m)}$, and after each $A^{(t)}$ is given we must estimate $\Tr(A^{(t)}ρ)$ to within $\pm ε$. This is the direct quantum generalization of the classical problem of \emph{Adaptive Data Analysis}. %The ``offline'' case, in which $A^{(1)}, \ldots, A^{(m)}$ are given upfront, is also a well-studied problem. The main goal is to minimize the number of copies, $n$, required. Prior results for online Shadow Tomography were suboptimal in all three parameters $m, d, ε$, lagging behind the best known and classical rates~\cite{bassily2021algorithmic}, for which there is some evidence of optimality. In this work, we finally close this gap, giving a pair of algorithms matching the classical rates. The bound on the left is the first to achieve $o(\log^2 m)$-dependence together with $\poly(\log(d)/\eps)$; moreover, it improves all three exponents even in the \emph{Offline} Shadow Tomography setting. The bound on the right is known to be optimal among bounds independent of~$d$, and improves the best prior result by a $\sqrt{m} \log m$ factor. The key to our proof is a new framework for quantifying post-measurement damage, based on the quantum Efron--Stein decomposition.