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arXiv:2610.40623

Optimal Diamond Distance Estimation for Unitary Channels

Jinge Bao, Qisheng Wang

quant-phSubmitted Oct 29, 2026• Announced Oct 30, 2026• 0 citations
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Abstract

The diamond distance between two quantum channels determines the optimal probability of distinguishing them from a single use. We give a quantum algorithm that estimates the diamond distance between two unknown $d$-dimensional unitary channels to within additive error $\varepsilon$, using $O(\sqrt{d}/\varepsilon)$ queries to the unitary channels and their inverses. The query complexity is optimal, as it matches the lower bound due to Jeon and Oh (npj Quantum Inf. 2026).

AI Summary

The paper studies additive-error estimation of the diamond distance between two unknown $d$-dimensional unitary channels, given query access to $U$, $V$, and their inverses. It gives an estimator with error at most $\varepsilon$ and success probability at least $2/3$ using $O(\sqrt d/\varepsilon)$ queries in the worst case, for $d\ge2$ and $0<\varepsilon\le1/4$. This improves the cited spectrum-estimation-based upper bound of $O(d\log^2 d/\varepsilon)$ and matches a known $\Omega(\sqrt d/\varepsilon)$ lower bound inherited from unitary channel certification. The construction uses the identity $\|\mathcal U-\mathcal V\|_\diamond=2\sin(\min\{\ell(U^\dagger V),\pi\}/2)$, where $\ell$ is the shortest spectral containing-arc length. A retained, unknown reference eigenvector and controlled-SWAP routing enable estimation of relative eigenphases without controlled access to the unknown unitaries. Bounded-error quantum search over eigenvector labels, initialized through a maximally entangled state, supplies comparisons for a multiscale interval search. Running this search in both phase directions estimates the truncated spectral width. Phase estimates near the wraparound cut are accepted conservatively; when this prevents two-sided phase accuracy, the diamond distance is already close to its maximum value of $2$, allowing the required final accuracy. Scale-dependent precision and failure probabilities avoid additional asymptotic logarithmic factors. The guarantee is specifically for unitary channels with inverse-query access and measures query complexity rather than total gate cost. It also reproduces the known $O(\sqrt d/\varepsilon)$ upper bound for promised unitary channel certification.

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12 pages, 4 figures, 1 algorithm

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The diamond distance between two quantum channels determines the optimal probability of distinguishing them from a single use. We give a quantum algorithm that estimates the diamond distance between two unknown ddd-dimensional unitary channels to within additive error ε\varepsilonε, using O(d/ε)O(\sqrt{d}/\varepsilon)O(d​/ε) queries to the unitary channels and their inverses. The query complexity is optimal, as it matches the lower bound due to Jeon and Oh (npj Quantum Inf. 2026).
The paper studies additive-error estimation of the diamond distance between two unknown ddd-dimensional unitary channels, given query access to UUU, VVV, and their inverses. It gives an estimator with error at most ε\varepsilonε and success probability at least 2/32/32/3 using O(d/ε)O(\sqrt d/\varepsilon)O(d​/ε) queries in the worst case, for d≥2d\ge2d≥2 and 0<ε≤1/40<\varepsilon\le1/40<ε≤1/4. This improves the cited spectrum-estimation-based upper bound of O(dlog⁡2d/ε)O(d\log^2 d/\varepsilon)O(dlog2d/ε) and matches a known Ω(d/ε)\Omega(\sqrt d/\varepsilon)Ω(d​/ε) lower bound inherited from unitary channel certification.
The construction uses the identity ∥U−V∥⋄=2sin⁡(min⁡{ℓ(U†V),π}/2)\|\mathcal U-\mathcal V\|_\diamond=2\sin(\min\{\ell(U^\dagger V),\pi\}/2)∥U−V∥⋄​=2sin(min{ℓ(U†V),π}/2), where ℓ\ellℓ is the shortest spectral containing-arc length. A retained, unknown reference eigenvector and controlled-SWAP routing enable estimation of relative eigenphases without controlled access to the unknown unitaries. Bounded-error quantum search over eigenvector labels, initialized through a maximally entangled state, supplies comparisons for a multiscale interval search. Running this search in both phase directions estimates the truncated spectral width. Phase estimates near the wraparound cut are accepted conservatively; when this prevents two-sided phase accuracy, the diamond distance is already close to its maximum value of 222, allowing the required final accuracy. Scale-dependent precision and failure probabilities avoid additional asymptotic logarithmic factors.
The guarantee is specifically for unitary channels with inverse-query access and measures query complexity rather than total gate cost. It also reproduces the known O(d/ε)O(\sqrt d/\varepsilon)O(d​/ε) upper bound for promised unitary channel certification.
We consider the problem of quantum channel certification to unitary, where one is given access to an unknown ddd-dimensional channel E\mathcal{E}E, and wants to test whether E\mathcal{E}E is equal to a target unitary channel or is ε\varepsilonε-far from it in the diamond norm. We present optimal quantum algorithms for this problem, settling the query complexities in three access models with increasing power. Specifically, we show that: (i) Θ(d/ε2)Θ(d/\varepsilon^2)Θ(d/ε2) queries suffice for incoherent access model, matching the lower bound due to Fawzi, Flammarion, Garivier, and Oufkir (COLT 2023). (ii) Θ(d/ε)Θ(d/\varepsilon)Θ(d/ε) queries suffice for coherent access model, matching the lower bound due to Regev and Schiff (ICALP 2008). (iii) Θ(d/ε)Θ(\sqrt{d}/\varepsilon)Θ(d​/ε) queries suffice for source-code access model, matching the lower bound due to Jeon and Oh (npj Quantum Inf. 2026). This demonstrates a strict hierarchy of complexities for quantum channel certification to unitary across various access models.
We consider process tomography for unitary quantum channels. Given access to an unknown unitary channel acting on a d-dimensional qudit, we aim to output a classical description of a unitary that is ε\varepsilonε-close to the unknown unitary in diamond norm. We design an algorithm achieving error ε\varepsilonε using O( d2/ε)O\left(\mathrm{~d}^{2} / \varepsilon\right)O( d2/ε) applications of the unknown channel and only one qudit. This improves over prior results, which use O( d3/ε2)O\left(\mathrm{~d}^{3} / \varepsilon^{2}\right)O( d3/ε2) [via standard process tomography] or O( d2.5/ε)O\left(\mathrm{~d}^{2.5} / \varepsilon\right)O( d2.5/ε) [Yang, Renner, and Chiribella, PRL 2020] applications. To show this result, we introduce a simple technique to “bootstrap” an algorithm that can produce constant-error estimates to one that can produce ε\varepsilonε-error estimates with the Heisenberg scaling. Finally, we prove a complementary lower bound showing that estimation requires Ω(d2/ε)\Omega\left(\mathrm{d}^{2} / \varepsilon\right)Ω(d2/ε) applications, even with access to the inverse or controlled versions of the unknown unitary. This shows that our algorithm has both optimal query complexity and optimal space complexity.
In the study of quantum process tomography, it has remained open how to learn a unitary channel in diamond distance with strictly parallel queries as efficiently as with sequential queries. Sequential queries allow one to exploit adaptivity to refine the estimate and adjust the learning strategy accordingly, whereas such adjustments are impossible for parallel queries. From the perspective of higher-order quantum operations, any parallel learning strategy can be simulated by a sequential one, whereas the converse does not hold in general, suggesting that sequential learning strategies are potentially more powerful. Contrary to this intuition, we present a new protocol for learning an unknown ddd-dimensional unitary channel to within ε\varepsilonε in diamond distance using O(d2/ε)\mathcal{O}(d^2/\varepsilon)O(d2/ε) parallel queries, matching the lower bound presented in [Haah, Kothari, O'Donnell, and Tang, FOCS '23]. Our protocol thus closes the gap between parallel and sequential strategies for unitary channel tomography. As applications, it achieves optimal query complexity for boundary-regime quantum channel tomography and improves the query efficiency of the best-known protocol for tomography of fermionic linear optics.
Quantum process tomography, the task of estimating an unknown quantum channel, is a central problem in quantum information theory. A long-standing open question is how many uses of an unknown channel are required to learn it in diamond distance, the standard metric for distinguishing quantum processes. While quantum state tomography is well understood, for general channels the problem remained open beyond the unitary case. Here we establish the query complexity of channel tomography with optimal dependence on the dimension parameters, at any fixed constant accuracy. We design an algorithm showing that any channel with input/output dimensions din,doutd_{\mathrm{in}},d_{\mathrm{out}}din​,dout​ and Kraus rank at most kkk can be learned to accuracy ε\varepsilonε using O(dindoutk/ε2)O(d_{\mathrm{in}}d_{\mathrm{out}}k/\varepsilon^{2})O(din​dout​k/ε2) channel uses. Conversely, we prove that Ω(dindoutk)Ω(d_{\mathrm{in}}d_{\mathrm{out}}k)Ω(din​dout​k) uses are necessary at constant accuracy and that, for non-minimal Kraus rank, a separate Ω(1/ε2)Ω(1/\varepsilon^{2})Ω(1/ε2) contribution is unavoidable. Since channels subsume states, unitaries, isometries, and measurements as special cases, our protocol provides a unified framework for these tomography tasks, yielding new guarantees for isometry and measurement tomography while recovering known optimal scalings for state and unitary tomography. Our algorithm follows the natural strategy of performing optimal tomography on the Choi state. The main technical contribution is to show that this suffices to control the induced diamond-distance error, avoiding the dimension loss incurred by a naive conversion from Choi-state trace distance to channel diamond distance. The protocol uses the channel non-adaptively to prepare Choi-state copies, purifies them in parallel, and performs optimal pure-state tomography on the resulting purifications. Hence, we reduce channel tomography to pure-state tomography.
We present fast algorithms $\unicode{x2013}$ under the depolarizing noise assumption, often made in fault-tolerant quantum computations $\unicode{x2013}$ to test its strength. Our optimal algorithms answer the following question: is the quantum channel implemented by a given black box identical to a target unitary or ε\varepsilonε-far from it in the diamond distance, assuming that the deviation is a depolarizing channel with unknown parameter? Our algorithm has a query complexity of Θ(1/ε).Θ(1/\varepsilon).Θ(1/ε). The query complexity of the relaxed problem of testing whether the black-box channel is ε1\varepsilon_1ε1​-close to a target unitary or ε2\varepsilon_2ε2​-far in the diamond distance is Θ(ε2/(ε2−ε1)2).Θ\bigl(\varepsilon_2/(\varepsilon_2 - \varepsilon_1)^2\bigr).Θ(ε2​/(ε2​−ε1​)2). In both cases, we provide matching lower bounds that hold even for adaptive, ancilla-assisted protocols with multi-outcome incoherent measurements.
We prove that learning an unknown quantum channel with input dimension dAd_AdA​, output dimension dBd_BdB​, and Choi rank rrr to diamond distance ε\varepsilonε requires $ Ω\!\left( \frac{d_A d_B r}{\varepsilon \log(d_B r / \varepsilon)} \right)$ channel queries when dA=rdBd_A= rd_BdA​=rdB​, and Ω ⁣(dAdBrε2log⁡(dBr/ε))Ω\!\left( \frac{d_A d_B r}{\varepsilon^2 \log(d_B r / \varepsilon)} \right)Ω(ε2log(dB​r/ε)dA​dB​r​) channel queries when dA≤rdB/2d_A\le rd_B/2dA​≤rdB​/2. These lower bounds improve upon the best previous Ω(dAdBr)Ω(d_A d_B r)Ω(dA​dB​r) bound by introducing explicit, near-optimal ε\varepsilonε-dependence. Moreover, when dA≤rdB/2d_A\le rd_B/2dA​≤rdB​/2, the lower bound is optimal up to a logarithmic factor. The proof constructs ensembles of channels that are well separated in diamond norm yet admit Stinespring isometries that are close in operator norm.