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The Power of Two Bases: Robust and copy-optimal certification of nearly all quantum states with few-qubit measurements

arXiv
Authors: Andrea Coladangelo, Jerry Li, Joseph Slote, Ellen Wu

Year

2026

Paper ID

86

Status

Preprint

Abstract Read

~2 min

Abstract Words

212

Citations

N/A

Abstract

A central task in quantum information science is state certification: testing whether an unknown state is ε1-close to a fixed target state, or ε2-far. Recent work has shown that surprisingly simple measurement protocols--comprising only single-qubit measurements--suffice to certify arbitrary n-qubit states [Huang, Preskill, Soleimanifar '25; Gupta, He, O'Donnell '25]. However, these certification protocols are not robust: rather than allowing constant ε1, they can only positively certify states within ε1=O(1/n) trace distance of the target. In many experimental settings, the appropriate error tolerance is constant as the system size grows, so this lack of robustness renders existing tests inapplicable at scale, no matter how many times the test is repeated. Here we present robust certification protocols based on few-qubit measurements that apply to all but a O\(2-n\)-fraction of pure target states. Our first protocol achieves constant robustness, i.e. ε1=Θ(1), using a single O\(log n\)-qubit measurement along with single-qubit measurements in the Z or X basis on the other qubits. As a corollary of its robustness, this protocol also achieves constant (in n) copy complexity, which is optimal. Our second protocol uses exclusively single-qubit measurements and is nearly robust: ε1=Ω\(1/log n\). Our tests are based on a new uncertainty principle for conditional fidelities, which may be of independent interest.

Why This Paper Matters

  • This paper contributes to the Benchmarking, Verification & Validation research area in the Quantum Articles archive.
  • It adds a 2026 reference point for readers tracking recent quantum research.
  • A central task in quantum information science is state certification: testing whether an unknown state is ε1-close to a fixed target state, or ε2-far.

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