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arXiv:2410.21201 · Leibniz international proceedings in informatics

Sample-Optimal Quantum Estimators for Pure-State Trace Distance and Fidelity via Samplizer

Qisheng Wang, Zhicheng Zhang

Published Oct 28, 2024• 0 citations
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Abstract

We settle the problem of estimating the trace distance and (square root) fidelity between $n$-qubit pure quantum states to within additive error $\varepsilon$, given their independent samples, which was raised as an open question by Wang (IEEE Trans. Inf. Theory 2024). This is achieved by a quantum algorithm with optimal sample complexity $Θ(1/\varepsilon^2)$, improving the long-standing folklore with sample complexity $O(1/\varepsilon^4)$. At the heart of our algorithm is a samplized phase estimation of the product of two Householder reflections. This is realized by an improved (multi-)samplizer for pure states, through which any quantum query algorithm using $Q$ queries to the reflection operator $I - 2|ψ\rangle\!\langleψ|$ can be converted to a $δ$-close (in the diamond norm distance) quantum sample algorithm using $Θ(Q^2/δ)$ samples of the state $|ψ\rangle$. This samplizer for pure states is also shown to be optimal.

DOI
10.4230/lipics.icalp.2026.154

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We settle the problem of estimating the trace distance and (square root) fidelity between nnn-qubit pure quantum states to within additive error ε\varepsilonε, given their independent samples, which was raised as an open question by Wang (IEEE Trans. Inf. Theory 2024). This is achieved by a quantum algorithm with optimal sample complexity Θ(1/ε2)Θ(1/\varepsilon^2)Θ(1/ε2), improving the long-standing folklore with sample complexity O(1/ε4)O(1/\varepsilon^4)O(1/ε4). At the heart of our algorithm is a samplized phase estimation of the product of two Householder reflections. This is realized by an improved (multi-)samplizer for pure states, through which any quantum query algorithm using QQQ queries to the reflection operator I−2∣ψ⟩ ⁣⟨ψ∣I - 2|ψ\rangle\!\langleψ|I−2∣ψ⟩⟨ψ∣ can be converted to a δδδ-close (in the diamond norm distance) quantum sample algorithm using Θ(Q2/δ)Θ(Q^2/δ)Θ(Q2/δ) samples of the state ∣ψ⟩|ψ\rangle∣ψ⟩. This samplizer for pure states is also shown to be optimal.
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Measuring the distinguishability between quantum states is a basic problem in quantum information theory. In this paper, we develop optimal quantum algorithms that estimate both the trace distance and the (square root) fidelity between pure states to within additive error$\varepsilon usingusingusing\Theta (1/\varepsilon)queriestotheirstate−preparationcircuits,quadraticallyimprovingthelong−standingfolklorequeries to their state-preparation circuits, quadratically improving the long-standing folklorequeriestotheirstate−preparationcircuits,quadraticallyimprovingthelong−standingfolkloreO(1/\varepsilon ^{2}) $. At the heart of our construction, is an algorithmic tool for quantum square root amplitude estimation, which generalizes the well-known quantum amplitude estimation.
The Uhlmann fidelity F(ρ0,ρ1)=tr∣ρ0ρ1∣{\rm F}(ρ_0,ρ_1) = {\rm tr}|\sqrt{ρ_0}\sqrt{ρ_1}|F(ρ0​,ρ1​)=tr∣ρ0​​ρ1​​∣ is one of the most fundamental quantities in quantum information theory for quantifying the closeness between two quantum states. Estimating the Uhlmann fidelity to within additive error ε\varepsilonε requires a number of copies of the states, or queries to their state-preparation circuits, that depends at least linearly on the smaller of the ranks of ρ0ρ_0ρ0​ and ρ1ρ_1ρ1​. Consequently, this rank dependence disappears when either state is pure, in which case the query and sample complexities depend only polynomially on 1/ε1/\varepsilon1/ε. However, the known optimal estimator for F(ρ,∣ψ⟩ ⁣⟨ψ∣){\rm F}(ρ,|ψ\rangle\!\langleψ|)F(ρ,∣ψ⟩⟨ψ∣) due to Fang and Wang (ESA 2025) requires prior knowledge of which state is pure. In this work, we remove this mathematically unnecessary prior-knowledge requirement and establish an optimal estimator for F(ρ,∣ψ⟩ ⁣⟨ψ∣){\rm F}(ρ, |ψ\rangle\!\langleψ|)F(ρ,∣ψ⟩⟨ψ∣) under the sole promise that one of the two states is pure, without knowing which one. Our estimator is obtained by specializing the refined algorithmic Uhlmann transform of Utsumi, Nakata, Wang, and Takagi (2025) to the case where one state is pure. In this setting, the Uhlmann fidelity can be recovered as follows: apply a unitary dilation of trA(∣ψ0⟩ ⁣⟨ψ1∣){\rm tr}_{\sf A}(|ψ_0\rangle\!\langleψ_1|)trA​(∣ψ0​⟩⟨ψ1​∣) (or its inverse) to the reference register R\sf RR of the purification ∣ψ1⟩|ψ_1\rangle∣ψ1​⟩ (or ∣ψ0⟩|ψ_0\rangle∣ψ0​⟩) on the registers A\sf AA and R\sf RR, estimate the corresponding square-root amplitude in each case, and take the maximum of the resulting two estimates.
Tight bounds on quantum sample complexity and quantum query complexity have been known for various computational problems in the literature, whereas tight bounds on quantum time complexity (i.e., the size of quantum circuits) remain unresolved. In this paper, we provide a framework to establish lower bounds on the quantum time complexity for testing permutation-invariant properties of quantum states, via a reduction from quantum sample complexity. As an application, we obtain a series of matching lower bounds when given sample access to the input quantum states, including: 1. The SWAP test due to Buhrman, Cleve, Watrous, and de Wolf (Phys. Rev. Lett. 2001) is time-optimal to estimate the purity tr⁡(ρ2)\operatorname{tr}(ρ^2)tr(ρ2) and the inner product tr⁡(ρσ)\operatorname{tr}(ρσ)tr(ρσ). 2. The Shift test due to Ekert, Alves, Oi, Horodecki, Horodecki, and Kwek (Phys. Rev. Lett. 2002) is time-optimal to estimate the high-order functionals tr⁡(ρk)\operatorname{tr}(ρ^k)tr(ρk). 3. The productness tester for multipartite pure states due to Harrow and Montanaro (J. ACM 2013) is time-optimal. 4. The LMR protocol due to Lloyd, Mohseni, and Rebentrost (Nat. Phys. 2014) is time-optimal to implement the reflection operator about a pure state. 5. The samplizer due to Wang and Zhang (IEEE Trans. Inf. Theory 2025) is time-optimal for pure states. 6. The estimator for pure-state trace distance and fidelity due to Wang and Zhang (ICALP 2026) is time-optimal. To the best of our knowledge, this is the first method that allows us to systematically establish tight lower bounds on quantum time complexity.
We consider the problem of estimating the fidelity of an unknown quantum state to a known reference state to within additive error ε\varepsilonε. We show that the sample complexity is O(r2/ε2)O(r^2/\varepsilon^2)O(r2/ε2) with optimal ε\varepsilonε-dependence when the reference state is of rank rrr, improving the previous best O(r2log⁡2(1/ε)/ε4)O(r^2\log^2(1/\varepsilon)/\varepsilon^4)O(r2log2(1/ε)/ε4) due to Utsumi, Nakata, Wang, and Takagi (QIP 2026). We also provide a lower bound of Ω(r/ε2)Ω(r/\varepsilon^2)Ω(r/ε2), improving the previous best Ω(r/ε+1/ε2)Ω(r/\varepsilon+1/\varepsilon^2)Ω(r/ε+1/ε2), with implications to quantum query complexity. Moreover, we further consider the case where the unknown state is of rank at most rrr while the reference state can be arbitrary, for which the sample complexity is shown to be O(r2/ε4)O(r^2/\varepsilon^4)O(r2/ε4). As an application, we present an approach to tolerant quantum state certification, generalizing the exact certification studied in Bădescu, O'Donnell, and Wright (STOC 2019).
We present an optimal quantum algorithm for fidelity estimation between two quantum states when one of them is pure. In particular, the (square root) fidelity of a mixed state to a pure state can be estimated to within additive error ε by using Θ(1/ε) queries to their state-preparation circuits, achieving a quadratic speedup over the folklore O(1/ε²). Our approach is technically simple, and can moreover estimate the quantity √{tr(ρσ²)} that is not common in the literature. To the best of our knowledge, this is the first query-optimal approach to fidelity estimation involving mixed states.