2020
DOI: 10.1103/physreva.102.022416
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Towards a realistic GaAs-spin qubit device for a classical error-corrected quantum memory

Abstract: Based on numerically optimized real-device gates and parameters we study the performance of the phase-flip (repetition) code on a linear array of gallium arsenide (GaAs) quantum dots hosting singlet-triplet qubits. We first examine the expected performance of the code using simple error models of circuit-level and phenomenological noise, reporting, for example, a circuit-level depolarizing noise threshold of approximately 3%. We then perform density-matrix simulations using a maximum-likelihood and minimum-wei… Show more

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Cited by 9 publications
(6 citation statements)
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“…1(a2). For the special case p sp = p id = p 1 = p m = p 2 = λ the threshold was found to lie at λ ≈ 0.033 for maximum likelihood decoding [61].…”
Section: Microscopic Circuit Noisementioning
confidence: 96%
“…1(a2). For the special case p sp = p id = p 1 = p m = p 2 = λ the threshold was found to lie at λ ≈ 0.033 for maximum likelihood decoding [61].…”
Section: Microscopic Circuit Noisementioning
confidence: 96%
“…1(a2). For the special case of uniform error probabilities (p sp = p id = p 1 = p m = p 2 = λ) the threshold was found to lie at λ ≈ 0.033 for maximum likelihood decoding [53].…”
Section: (A1)mentioning
confidence: 98%
“…For example, quantum error correction (QEC) has the goal of introducing protocols to detect and correct those errors. However, its implementation is currently challenging and it requires certain thresholds for it to be feasible [19][20][21][22]. The QEC scheme to be applied depends on the characteristics of the noise and the presence of spatial correlations can be severely detrimental [23][24][25][26][27][28][29][30].…”
Section: Introductionmentioning
confidence: 99%