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arXiv:2607.13476

Quantum memory advantage for quantum process tomography

Carlos Bravo-Prieto, Weiyuan Gong, Antonio Anna Mele

quant-phcs.DSmath-phSubmitted Jul 15, 2026• Announced Jul 16, 2026• 0 citations
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Abstract

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 $Θ(d_{\mathrm{in}}^3 d_{\mathrm{out}}^3/\varepsilon^2)$, where $d_{\mathrm{in}}$ and $d_{\mathrm{out}}$ are the channel input and output dimensions, respectively, and $\varepsilon$ is the target diamond-norm accuracy. More precisely, we prove that any incoherent protocol for this task, including adaptive protocols, requires $Ω(d_{\mathrm{in}}^3 d_{\mathrm{out}}^3/\varepsilon^2)$ 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 $O(d_{\mathrm{in}}^3 d_{\mathrm{out}}^3/\varepsilon^2)$. Our results thereby generalize the optimal sample-complexity bounds for single-copy state tomography, recovered as the special case $d_{\mathrm{in}}=1$. By contrast, coherent protocols with quantum memory achieve query complexity $Θ(d_{\mathrm{in}}^2 d_{\mathrm{out}}^2/\varepsilon^2)$. Hence, our results establish a rigorous learning separation between quantum process tomography with and without quantum memory.

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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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We study tomography for quantum channels with input dimension d1d_1d1​, output dimension d2d_2d2​, and Kraus rank at most rrr, to within diamond norm error ε\varepsilonε, using adaptive experiments that retain no quantum memory between channel queries. - For quantum channels whose non-zero Choi eigenvalues are bounded below by Ω(d1/r)Ω(d_1/r)Ω(d1​/r), we establish optimal query upper and lower bounds Θ(d1d2r2/ε2)Θ(d_1d_2r^2/ε^2)Θ(d1​d2​r2/ε2). The upper bound is achieved by a nonadaptive algorithm that uses the estimator from [Surawy-Stepney et al., Quantum (2022)], together with a new diamond-norm analysis. The lower bound applies to arbitrary adaptive incoherent protocols and follows from a new local family of channels and a uniform one-query Fisher-information bound. - For general channels, we establish an upper bound O(d1d2r2log⁡(2d1)/ε2)O(d_1d_2r^2\log(2d_1)/ε^2)O(d1​d2​r2log(2d1​)/ε2), nearly matching the above lower bound Ω(d1d2r2/ε2)Ω(d_1d_2r^2/\varepsilon^2)Ω(d1​d2​r2/ε2). To achieve this, we generalize the above nonadaptive algorithm by adapting the input state over O(log⁡(2d1))O(\log(2d_1))O(log(2d1​)) rounds with the Matrix Multiplicative Weight Update algorithm.
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.
How many copies of a quantum process are necessary and sufficient to construct an approximate classical description of it? We extend the result of Surawy-Stepney, Kahn, Kueng, and Guta (2022) to show that O~(d6/ε2){\tilde {\mathcal{O}}}\left( {{d^6}/{\varepsilon ^2}} \right)O~(d6/ε2) copies are sufficient to learn a d-dimensional quantum channel to within ε in the diamond norm. Moreover, we show that Ω(d6/ε2) copies are necessary for any strategy using incoherent non-adaptive measurements. This lower bound applies even for ancilla-assisted strategies.
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.
Learning about physical systems from quantum-enhanced experiments can outperform learning from experiments in which only classical memory and processing are available. Whereas quantum advantages have been established for state learning, quantum process learning is less understood. We establish an exponential quantum advantage for learning an unknown n -qubit quantum process N\mathcal {N}N . We show that a quantum memory allows to efficiently solve the following tasks: (a) learning the Pauli transfer matrix (PTM) of an arbitrary N\mathcal {N}N , (b) predicting expectation values of Pauli-sparse observables measured on the output of an arbitrary N\mathcal {N}N upon input of a Pauli-sparse state, and (c) predicting expectation values of arbitrary observables measured on the output of an unknown N\mathcal {N}N with sparse PTM upon input of an arbitrary state. With quantum memory, these tasks can be solved using linearly-in- n many copies of the Choi state of N\mathcal {N}N . In contrast, any learner without quantum memory requires exponentially-in- n many queries, even when using adaptively designed experiments. In proving this separation, we extend existing shadow tomography bounds from states to channels. Moreover, we combine PTM learning with polynomial interpolation to learn arbitrary Hamiltonians from short-time dynamics. Our results highlight the power of quantum-enhanced experiments for learning highly complex quantum dynamics.