2018
DOI: 10.1002/qute.201800012
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Adaptive Weight Estimator for Quantum Error Correction in a Time‐Dependent Environment

Abstract: Quantum error correction of a surface code or repetition code requires the pairwise matching of error events in a space‐time graph of qubit measurements, such that the total weight of the matching is minimized. The input weights follow from a physical model of the error processes that affect the qubits. This approach becomes problematic if the system has sources of error that change over time. Here, it is shown that the weights can be determined from the measured data in the absence of an error model. The resu… Show more

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Cited by 15 publications
(16 citation statements)
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“…The occurrence of an error is signaled by d n ½ ¼ 1. To pair defects we use a minimum-weight perfectmatching (MWPM) decoder, whose weights are trained on simulated data without leakage 27,48 and we benchmark its logical performance in the presence of leakage errors. The logical qubit is initialized in 0 j i L and the logical fidelity is calculated at each QEC cycle, from which the logical error rate ε L can be extracted 27 .…”
Section: Effect Of Leakage On the Code Performancementioning
confidence: 99%
See 1 more Smart Citation
“…The occurrence of an error is signaled by d n ½ ¼ 1. To pair defects we use a minimum-weight perfectmatching (MWPM) decoder, whose weights are trained on simulated data without leakage 27,48 and we benchmark its logical performance in the presence of leakage errors. The logical qubit is initialized in 0 j i L and the logical fidelity is calculated at each QEC cycle, from which the logical error rate ε L can be extracted 27 .…”
Section: Effect Of Leakage On the Code Performancementioning
confidence: 99%
“…For the Surface-17 simulations we use the open-source density-matrix simulation package quantumsim 27 , available at "The quantumsim package can be found at https://quantumsim.gitlab.io/". For decoding we use a MWPM decoder 27 , for which the weights of the possible error pairings are extracted from Surface-17 simulations via adaptive estimation 48 without leakage (L 1 = 0) and an otherwise identical error model (described in section "Error model and parameters").…”
Section: Simulation Protocolmentioning
confidence: 99%
“…For the Surface-17 simulations we use the open-source density-matrix simulation package quantumsim [27], available at [47]. For decoding we use a MWPM decoder [27], for which the weights of the possible error pairings are extracted from Surface-17 simulations via adaptive estimation [56] without leakage (L 1 = 0) and an otherwise identical error model (described in Appendix B).…”
Section: Discussionmentioning
confidence: 99%
“…Ancilla-qubit measurements are modeled as projective in the {|0 , |1 , |2 } basis and ancilla qubits are not reset between QEC cycles. As a consequence, given the ancilla-qubit mea- decoder, whose weights are trained on simulated data without leakage [27,49] and we benchmark its logical performance in the presence of leakage errors. The logical qubit is initialized in |0 L and the logical fidelity is calculated at each QEC cycle, from which the logical error rate ε L can be extracted [27].…”
Section: B Effect Of Leakage On the Code Performancementioning
confidence: 99%
“…We determine the weights in an error-model-free approach by inferring the errors per cycle from the measured data using a correlation analysis of the syndromes as described in Appendix L and Refs. [9,50]. The correction of an error, initiated by analysing all cycles in postprocessing, takes the form of changing the sign of the logical qubit operator values z L and x L when indicated by the decoder.…”
Section: Repeated Quantum Error Correctionmentioning
confidence: 99%