Non-iid hypothesis testing: from classical to quantum
October 07, 2025 Β· Declared Dead Β· π arXiv.org
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Authors
Giacomo De Palma, Marco Fanizza, Connor Mowry, Ryan O'Donnell
arXiv ID
2510.06147
Category
quant-ph: Quantum Computing
Cross-listed
cs.DS,
cs.LG
Citations
0
Venue
arXiv.org
Last Checked
5 months ago
Abstract
We study hypothesis testing (aka state certification) in the non-identically distributed setting. A recent work (Garg et al. 2023) considered the classical case, in which one is given (independent) samples from $T$ unknown probability distributions $p_1, \dots, p_T$ on $[d] = \{1, 2, \dots, d\}$, and one wishes to accept/reject the hypothesis that their average $p_{\mathrm{avg}}$ equals a known hypothesis distribution $q$. Garg et al. showed that if one has just $c = 2$ samples from each $p_i$, and provided $T \gg \frac{\sqrt{d}}{Ξ΅^2} + \frac{1}{Ξ΅^4}$, one can (whp) distinguish $p_{\mathrm{avg}} = q$ from $d_{\mathrm{TV}}(p_{\mathrm{avg}},q) > Ξ΅$. This nearly matches the optimal result for the classical iid setting (namely, $T \gg \frac{\sqrt{d}}{Ξ΅^2}$). Besides optimally improving this result (and generalizing to tolerant testing with more stringent distance measures), we study the analogous problem of hypothesis testing for non-identical quantum states. Here we uncover an unexpected phenomenon: for any $d$-dimensional hypothesis state $Ο$, and given just a single copy ($c = 1$) of each state $Ο_1, \dots, Ο_T$, one can distinguish $Ο_{\mathrm{avg}} = Ο$ from $D_{\mathrm{tr}}(Ο_{\mathrm{avg}},Ο) > Ξ΅$ provided $T \gg d/Ξ΅^2$. (Again, we generalize to tolerant testing with more stringent distance measures.) This matches the optimal result for the iid case, which is surprising because doing this with $c = 1$ is provably impossible in the classical case. We also show that the analogous phenomenon happens for the non-iid extension of identity testing between unknown states. A technical tool we introduce may be of independent interest: an Efron-Stein inequality, and more generally an Efron-Stein decomposition, in the quantum setting.
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