Abstract

Quantum error correction allows to actively correct errors occurring in a quantum computation when the noise is weak enough. To make this error correction competitive information about the specific noise is required. Traditionally, this information is obtained by benchmarking the device before operation. We address the question of what can be learned from only the measurements done during decoding. Such estimation of noise models was proposed for surface codes, exploiting their special structure, and in the limit of low error rates also for other codes. However, so far it has been unclear under what general conditions noise models can be estimated from the syndrome measurements. In this work, we derive a general condition for identifiability of the error rates. For general stabilizer codes, we prove identifiability under the assumption that the rates are small enough. Without this assumption we prove a result for perfect codes. Finally, we propose a practical estimation method with linear runtime for concatenated codes. We demonstrate that it outperforms other recently proposed methods and that the estimation is optimal in the sense that it reaches the Cram\'{e}r-Rao Bound. Our method paves the way for practical calibration of error corrected quantum devices during operation.

Highlights

  • Quantum error correction is an essential ingredient in quantum computing schemes

  • We investigated the estimation of stochastic error models from the syndrome statistics of a quantum error correction code, establishing both theoretical results on parameter identifiability as well as a practical estimation method

  • The results do not rely on the limit of low error rates, and our estimator outperforms other recently proposed methods [2,3,4]

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Summary

INTRODUCTION

Quantum error correction is an essential ingredient in quantum computing schemes. When employing active quantum error correction via stabilizer codes, the decoding can be significantly improved if information about the error rates of all qubits is available. As pointed out by Fowler et al [2], this results in a noise model that is directly applicable for the decoder It allows for the tracking of timevarying error rates [3,6]. Models, including surface codes with independent Pauli noise on each qubit, the analytical method developed by [6] proves parameter identifiability. We introduce an explicit error rates estimator, similar to techniques employed in classical distributed source coding [12], for concatenated codes and simulate it on the concatenated five-qubit code. The Pauli operator acting as e ∈ P1 on qubit i and as the identity elsewhere is denoted e(i) ∈ Pn. A stabilizer code encoding k = n − l qubits is defined by a commutative subgroup S of Pn with generators g1, .

IDENTIFIABILITY CONDITIONS
NUMERICAL ESTIMATION METHOD
Belief propagation
Expectation maximization
Numerical results
Analytical solution under a conditional independence assumption
Formal definition of error model
Proof of theorem 3
Proof of lemma 6
MSE of the estimator
Estimator with measurement noise
CONCLUSION
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