Fast quantum measurement tomography with optimal error bounds
1ICFO – Institut de Ciències Fotòniques, The Barcelona Institute of Science and Technology, 08860 Castelldefels, Barcelona, Spain
2Centre for Quantum Technologies, National University of Singapore, Singapore.
3Quantum Research Center, Technology Innovation Institute, Abu Dhabi, UAE
4Department of Quantum Information and Computation at Kepler (QUICK), Johannes Kepler University Linz, 4040 Linz, Austria
| Published: | 2026-07-15, volume 10, page 2162 |
| Editor: | Jiangwei Shang |
| Eprint: | arXiv:2507.04500v3 |
| Doi: | https://doi.org/10.22331/q-2026-07-15-2162 |
| Citation: | Quantum 10, 2162 (2026). |
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Abstract
We present a two-step protocol for quantum measurement tomography that is light on classical co-processing cost and still achieves optimal sample complexity. Given measurement data from a known probe state ensemble, we first apply least-squares estimation to produce an unconstrained approximation of the POVM, and then project this estimate onto the set of valid quantum measurements. For a POVM with $L$ outcomes acting on a $d$-dimensional system, we show that the protocol requires $\mathcal{O}\left((d^3+d^2L)/\epsilon^2\right)$ samples to achieve error $\epsilon$ in worst-case distance, and $\mathcal{O}(d^2 L/\epsilon^2)$ samples in average-case distance. We further establish two matching sample complexity lower bounds of $\Omega((d^3 + d^2 L) /\epsilon^2)$ and $\Omega(d^2 L/\epsilon^2)$ for any non-adaptive, single-copy POVM tomography protocol. Hence, our projected least squares POVM tomography is sample-optimal in both the dimension and the number of outcomes for both distances. Our method admits an analytic form when using global or local 2-designs as probe ensembles and enables rigorous non-asymptotic error guarantees. Finally, we also complement our findings with empirical performance studies carried out on a noisy superconducting quantum computer with flux-tunable transmon qubits.
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