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arXiv:2512.10214

Optimal learning of quantum channels in diamond distance

Antonio Anna Mele, Lennart Bittel

quant-phcs.CCcs.DSSubmitted Dec 11, 2025• Announced Dec 12, 2025• 0 citations• Revised Jan 16, 2026 (v2)
v1 · Dec 11, 2025v2 · Jan 16, 2026v3 · Jun 15, 2026
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Abstract

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 to determine the optimal number of uses of an unknown channel required to learn it in diamond distance, the standard metric for distinguishing quantum processes. While the analogous problem of quantum state tomography has been settled over the past decades in both the pure- and mixed-state settings, for general quantum channels it remained largely open beyond the unitary case. Here we design an algorithm showing that any channel with input and output dimensions $d_{\mathrm{in}},d_{\mathrm{out}}$ and Kraus rank at most $k$ can be learned to constant accuracy in diamond distance using $Θ(d_{\mathrm{in}}d_{\mathrm{out}}k)$ channel uses, and we prove that this scaling is optimal via a matching lower bound. More generally, achieving accuracy $\varepsilon$ is possible with $O(d_{\mathrm{in}}d_{\mathrm{out}}k/\varepsilon^{2})$ channel uses. Since quantum channels subsume states, unitaries, and isometries as special cases, our protocol provides a unified framework for the corresponding tomography tasks; in particular, it yields the first optimal protocols for isometries and for binary measurement tomography, and it recovers optimal trace-distance tomography for fixed-rank states. Our approach reduces channel tomography to pure-state tomography: we use the channel to prepare copies of its Choi state, purify them in parallel, and run sample-optimal pure-state tomography on the resulting purifications; we then show that the induced diamond-distance error scales essentially linearly with the trace-distance error in estimating the (purified) Choi state. We also resolve an open question by showing that adaptivity does not improve the dimension-optimal query complexity of quantum channel tomography.

Comments
10 + 43 pages, 1 figure. Added a section on query-complexity lower bounds

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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 to determine the optimal number of uses of an unknown channel required to learn it in diamond distance, the standard metric for distinguishing quantum processes. While the analogous problem of quantum state tomography has been settled over the past decades in both the pure- and mixed-state settings, for general quantum channels it remained largely open beyond the unitary case. Here we design an algorithm showing that any channel with input and output dimensions din,doutd_{\mathrm{in}},d_{\mathrm{out}}din​,dout​ and Kraus rank at most kkk can be learned to constant accuracy in diamond distance using Θ(dindoutk)Θ(d_{\mathrm{in}}d_{\mathrm{out}}k)Θ(din​dout​k) channel uses, and we prove that this scaling is optimal via a matching lower bound. More generally, achieving accuracy ε\varepsilonε is possible with O(dindoutk/ε2)O(d_{\mathrm{in}}d_{\mathrm{out}}k/\varepsilon^{2})O(din​dout​k/ε2) channel uses. Since quantum channels subsume states, unitaries, and isometries as special cases, our protocol provides a unified framework for the corresponding tomography tasks; in particular, it yields the first optimal protocols for isometries and for binary measurement tomography, and it recovers optimal trace-distance tomography for fixed-rank states. Our approach reduces channel tomography to pure-state tomography: we use the channel to prepare copies of its Choi state, purify them in parallel, and run sample-optimal pure-state tomography on the resulting purifications; we then show that the induced diamond-distance error scales essentially linearly with the trace-distance error in estimating the (purified) Choi state. We also resolve an open question by showing that adaptivity does not improve the dimension-optimal query complexity of quantum channel tomography.
How many black-box queries to a quantum channel are needed to learn its full classical description? This question lies at the heart of quantum channel tomography (also known as quantum process tomography), a fundamental task in the characterization and validation of quantum hardware. Despite extensive prior work, the optimal query complexity for quantum channel tomography is far from fully understood. In this paper, we study tomography of an unknown quantum channel with input dimension d1d_1d1​, output dimension d2d_2d2​, and Kraus rank at most rrr, to within error ε\varepsilonε. We identify the dilation rate τ=rd2/d1τ= r d_2 / d_1τ=rd2​/d1​ (which always satisfies τ≥1τ\geq 1τ≥1 due to the trace preservation of quantum channels) as a key parameter, and establish that the optimal query complexity of channel tomography exhibits distinct scaling laws across three regimes of τττ. - In the boundary regime (τ=1τ= 1τ=1): we show that the query complexity is Θ(rd1d2/ε)Θ(r d_1 d_2/\varepsilon)Θ(rd1​d2​/ε) for Choi trace norm error ε\varepsilonε, and is upper bounded by O(min⁡{rd11.5d2/ε,rd1d2/ε2})O(\min\{r d_1^{1.5} d_2/\varepsilon, r d_1 d_2/\varepsilon^2\})O(min{rd11.5​d2​/ε,rd1​d2​/ε2}) and lower bounded by Ω(rd1d2/ε)Ω(r d_1 d_2/\varepsilon)Ω(rd1​d2​/ε) for diamond norm error ε\varepsilonε. - In the away-from-boundary regime (τ≥1+Ω(1)τ\geq 1+Ω(1)τ≥1+Ω(1)): we show that the query complexity is Θ(rd1d2/ε2)Θ(r d_1 d_2/\varepsilon^2)Θ(rd1​d2​/ε2) for both Choi trace norm and diamond norm errors ε\varepsilonε. Our results uncover a sharp Heisenberg-to-classical phase transition in the query complexity of quantum channel tomography: at τ=1τ=1τ=1, the optimal query complexity exhibits Heisenberg scaling 1/ε1/\varepsilon1/ε, whereas for τ≥1+Ω(1)τ\geq 1+Ω(1)τ≥1+Ω(1), it exhibits classical scaling 1/ε21/\varepsilon^21/ε2. In addition, we show that in the near-boundary regime (1<τ<1+o(1)1< τ< 1+o(1)1<τ<1+o(1)), the query complexity exhibits a mixture of Heisenberg and classical scaling behaviors.
We give collective tomography protocols for quantum states and channels with known symmetries, using random purification and dilation to reduce learning to pure-state estimation. For states commuting with a compact-group representation with multiplicities mλm_λmλ​, the optimal copy complexity is Θ((∑λmλ2+log⁡η−1)/ε2)Θ((\sum_λm_λ^2+\logη^{-1})/\varepsilon^2)Θ((∑λ​mλ2​+logη−1)/ε2) for sufficiently small trace-distance error ε\varepsilonε and failure probability ηηη for the nontrivial case ∑λmλ2>1\sum_λm_λ^2>1∑λ​mλ2​>1. For GGG-covariant channels with finite-dimensional unitary representations of a compact group GGG, parallel O~(DG/ε2)\widetilde{O}(D_G/\varepsilon^2)O(DG​/ε2) queries achieve a diamond-distance error $\varepsilon $ at fixed success probability 2/32/32/3, where DGD_GDG​ counts the real parameters of covariant Choi operators before imposing trace preservation. For permutation-covariant channels on kkk qudits of fixed local dimension ddd, at sufficiently small fixed error and fixed success probability 2/32/32/3, we obtain the optimal query scalings Θd(kd4−1)Θ_d(k^{d^4-1})Θd​(kd4−1) for diamond distance and Θd(kd4−d2)Θ_d(k^{d^4-d^2})Θd​(kd4−d2) for Choi trace distance. Furthermore, we resolve an open problem in quantum tomography of constructing efficient quantum circuits that approximate the Hayashi measurement for optimal pure-state estimation. We encode states in the symmetric subspace into bosonic occupation modes, realize the measurement by heterodyne detection and normalization, and approximate this procedure on qubits using the quantum Hermite transform. Combined with our symmetry-compatible purification and dilation circuits, this yields query-optimal and gate-efficient learners of permutation-covariant states and channels with gate complexity Od(poly(k,ε−1,log⁡η−1))O_d(\mathrm{poly}(k,\varepsilon^{-1},\logη^{-1}))Od​(poly(k,ε−1,logη−1)).
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.
We study the estimation of an unknown quantum channel E\mathcal{E}E with input dimension d1d_1d1​, output dimension d2d_2d2​ and Kraus rank at most rrr. We establish a connection between the query complexities in two models: (i) access to E\mathcal{E}E, and (ii) access to a random dilation of E\mathcal{E}E. Specifically, we show that for parallel (possibly coherent) testers, access to dilations does not help. This is proved by constructing a local tester that uses nnn queries to E\mathcal{E}E yet faithfully simulates the tester with nnn queries to a random dilation. As application, we show that: - O(rd1d2/ε2)O(rd_1d_2/\varepsilon^2)O(rd1​d2​/ε2) queries to E\mathcal{E}E suffice for channel tomography to within diamond norm error ε\varepsilonε. Moreover, when rd2=d1rd_2=d_1rd2​=d1​, we show that the Heisenberg scaling O(1/ε)O(1/\varepsilon)O(1/ε) can be achieved, even if E\mathcal{E}E is not a unitary channel: - O(min⁡{d12.5/ε,d12/ε2})O(\min\{d_1^{2.5}/\varepsilon,d_1^2/\varepsilon^2\})O(min{d12.5​/ε,d12​/ε2}) queries to E\mathcal{E}E suffice for channel tomography to within diamond norm error ε\varepsilonε, and O(d12/ε)O(d_1^2/\varepsilon)O(d12​/ε) queries suffice for the case of Choi state trace norm error ε\varepsilonε. - O(min⁡{d11.5/ε,d1/ε2})O(\min\{d_1^{1.5}/\varepsilon,d_1/\varepsilon^2\})O(min{d11.5​/ε,d1​/ε2}) queries to E\mathcal{E}E suffice for tomography of the mixed state E(∣0⟩⟨0∣)\mathcal{E}(|0\rangle\langle 0|)E(∣0⟩⟨0∣) to within trace norm error ε\varepsilonε.
Quantum process tomography, the task of learning an unknown quantum channel from black-box access, is a central problem in quantum information. In this setting, protocols with quantum memory can coherently store and jointly process quantum information obtained from multiple channel uses, whereas protocols without quantum memory must measure after each use and retain only a classical transcript of the measurement outcomes. A fundamental open question is whether quantum memory provides a query-complexity advantage even when protocols without quantum memory may adapt their experiments based on all previous outcomes with unbounded classical computational power. In this work, we show that it does. We determine the optimal query complexity of quantum process tomography without quantum memory up to a constant factor to be Θ(din3dout3/ε2)Θ(d_{\mathrm{in}}^3 d_{\mathrm{out}}^3/\varepsilon^2)Θ(din3​dout3​/ε2), where dind_{\mathrm{in}}din​ and doutd_{\mathrm{out}}dout​ are the channel input and output dimensions, respectively, and ε\varepsilonε is the target diamond-norm accuracy. More precisely, we prove that any incoherent protocol for this task, including adaptive protocols, requires Ω(din3dout3/ε2)Ω(d_{\mathrm{in}}^3 d_{\mathrm{out}}^3/\varepsilon^2)Ω(din3​dout3​/ε2) queries, even when each channel use may be assisted by arbitrary fresh ancilla, and we present a non-adaptive, ancilla-free incoherent protocol achieving the matching upper bound O(din3dout3/ε2)O(d_{\mathrm{in}}^3 d_{\mathrm{out}}^3/\varepsilon^2)O(din3​dout3​/ε2). Our results thereby generalize the optimal sample-complexity bounds for single-copy state tomography, recovered as the special case din=1d_{\mathrm{in}}=1din​=1. By contrast, coherent protocols with quantum memory achieve query complexity Θ(din2dout2/ε2)Θ(d_{\mathrm{in}}^2 d_{\mathrm{out}}^2/\varepsilon^2)Θ(din2​dout2​/ε2). Hence, our results establish a rigorous learning separation between quantum process tomography with and without quantum memory.
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