🤖 AI Summary
This work investigates the sample complexity lower bounds for estimating unitarily invariant properties of high-dimensional quantum states, including spectral estimation, von Neumann entropy estimation, and rank testing. By constructing hard instances of mixed states based on normalized Haar-random projectors and innovatively employing Jucys–Murphy elements from the symmetric group algebra—along with their higher-order symmetric functions—to analyze quantum state moments and indistinguishability, the authors combine moment matching with f-divergence bounds to establish, for the first time, nearly tight lower bounds of Ω(d²⁻ᵞ) under constant error. These results demonstrate that the sample complexity of these tasks is nearly as demanding as that of full quantum state tomography.
📝 Abstract
We study the sample complexity of estimating and testing fundamental unitarily invariant properties of unknown quantum states; namely, the tasks of spectrum estimation, von Neumann entropy estimation, and rank-testing. For $d$-dimensional states, and for every $γ>0$, we prove a sample complexity lower bound of $Ω(d^{2-γ})$ for spectrum estimation to constant sorted total-variation error, entropy estimation to constant additive error, and rank-testing to constant trace distance. Our hard instances are constructed from sandwiched products of Haar-random projectors, suitably normalized using a novel technique that lets us derive explicit expressions for high-order tensor moments of the resultant states. These moments can be expressed as symmetric functions of Jucys--Murphy elements of the symmetric group algebra. To show that two such mixtures are indistinguishable, we analyze the log-likelihood ratio and perform moment-matching, i.e., we set its low-order Jucys--Murphy components to zero. Indistinguishability is then obtained by bounding an $f$-divergence through the high-order components; the non-zero high-order terms and concentration of functions of Haar-random unitaries also imply separations in typical spectra, entropies, and ranks, proving all our lower bounds.