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Inverse-free quantum state estimation with Heisenberg scaling

Kean Chen

TL;DR

This work investigates inverse-free quantum state and amplitude estimation under query access, showing that Heisenberg-scaling results can be achieved using only forward queries. The authors construct a probe state based on Gamma-shaped Young tableaux and extract the last-column information of the unknown unitary $U$ via a pretty good measurement, achieving an error bound that scales as $O(d^3/(n^2+nd^2))$ and translating to a forward-query complexity of $O\big(\min\{d^{3/2}/\varepsilon, d/\varepsilon^2\}\big)$ for estimating $U|d\rangle$ within $\varepsilon$. They further derive inverse-free bounds for amplitude estimation, namely $O\big(\min\{d^{3/2}/\varepsilon,1/\varepsilon^2\}\big)$, improving previous results and contradicting a conjecture that inverse access is necessary for optimal inverse-free scaling. The results illuminate how inverse access affects different quantum-estimation tasks and demonstrate that Heisenberg scaling can be achieved without incurring a quadratic-dimension overhead in the inverse-free setting.

Abstract

In this paper, we present an inverse-free pure quantum state estimation protocol that achieves Heisenberg scaling. Specifically, let $\mathcal{H}\cong \mathbb{C}^d$ be a $d$-dimensional Hilbert space with an orthonormal basis $\{|1\rangle,\ldots,|d\rangle\}$ and $U$ be an unknown unitary on $\mathcal{H}$. Our protocol estimates $U|d\rangle$ to within trace distance error $\varepsilon$ using $O(\min\{d^{3/2}/\varepsilon,d/\varepsilon^2\})$ forward queries to $U$. This complements the previous result $O(d\log(d)/\varepsilon)$ by van Apeldoorn, Cornelissen, Gilyén, and Nannicini (SODA 2023), which requires both forward and inverse queries. Moreover, our result implies a query upper bound $O(\min\{d^{3/2}/\varepsilon,1/\varepsilon^2\})$ for inverse-free amplitude estimation, improving the previous best upper bound $O(\min\{d^{2}/\varepsilon,1/\varepsilon^2\})$ based on optimal unitary estimation by Haah, Kothari, O'Donnell, and Tang (FOCS 2023), and disproving a conjecture posed in Tang and Wright (2025).

Inverse-free quantum state estimation with Heisenberg scaling

TL;DR

This work investigates inverse-free quantum state and amplitude estimation under query access, showing that Heisenberg-scaling results can be achieved using only forward queries. The authors construct a probe state based on Gamma-shaped Young tableaux and extract the last-column information of the unknown unitary via a pretty good measurement, achieving an error bound that scales as and translating to a forward-query complexity of for estimating within . They further derive inverse-free bounds for amplitude estimation, namely , improving previous results and contradicting a conjecture that inverse access is necessary for optimal inverse-free scaling. The results illuminate how inverse access affects different quantum-estimation tasks and demonstrate that Heisenberg scaling can be achieved without incurring a quadratic-dimension overhead in the inverse-free setting.

Abstract

In this paper, we present an inverse-free pure quantum state estimation protocol that achieves Heisenberg scaling. Specifically, let be a -dimensional Hilbert space with an orthonormal basis and be an unknown unitary on . Our protocol estimates to within trace distance error using forward queries to . This complements the previous result by van Apeldoorn, Cornelissen, Gilyén, and Nannicini (SODA 2023), which requires both forward and inverse queries. Moreover, our result implies a query upper bound for inverse-free amplitude estimation, improving the previous best upper bound based on optimal unitary estimation by Haah, Kothari, O'Donnell, and Tang (FOCS 2023), and disproving a conjecture posed in Tang and Wright (2025).

Paper Structure

This paper contains 23 sections, 6 theorems, 63 equations, 2 figures, 1 table, 1 algorithm.

Key Result

Theorem 1.2

There is a quantum protocol that uses $n$ forward queries to $U$ and outputs a classical description of a unit vector $\lvert\psi\rangle$. The output $\lvert\psi\rangle$ is random and satisfies

Figures (2)

  • Figure 1: Definition of the semistandard Young tableaux $\Gamma_i$ and $\Gamma_i^+$.
  • Figure 2: The decomposition of $\lvert\Gamma_i\rangle\otimes \lvert d\rangle$

Theorems & Definitions (17)

  • Theorem 1.2
  • Corollary 1.3
  • proof
  • Corollary 1.5
  • proof
  • Definition 3.1: $\Gamma$-shaped tableaux
  • Definition 3.2: The probe state
  • Lemma 4.1
  • proof
  • Lemma 4.2
  • ...and 7 more