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Published July 2021 | Published + Accepted Version
Journal Article Open

Quantum Coding with Low-Depth Random Circuits

Abstract

Random quantum circuits have played a central role in establishing the computational advantages of near-term quantum computers over their conventional counterparts. Here, we use ensembles of low-depth random circuits with local connectivity in D ≥ 1 spatial dimensions to generate quantum error-correcting codes. For random stabilizer codes and the erasure channel, we find strong evidence that a depth O(log N) random circuit is necessary and sufficient to converge (with high probability) to zero failure probability for any finite amount below the optimal erasure threshold, set by the channel capacity, for any D. Previous results on random circuits have only shown that O(N^(1/D)) depth suffices or that O(log³ N) depth suffices for all-to-all connectivity (D → ∞). We then study the critical behavior of the erasure threshold in the so-called moderate deviation limit, where both the failure probability and the distance to the optimal threshold converge to zero with N. We find that the requisite depth scales like O(log N) only for dimensions D ≥ 2 and that random circuits require O(√N) depth for D = 1. Finally, we introduce an "expurgation" algorithm that uses quantum measurements to remove logical operators that cause the code to fail by turning them into either additional stabilizers or into gauge operators in a subsystem code. With such targeted measurements, we can achieve sublogarithmic depth in D ≥ 2 spatial dimensions below capacity without increasing the maximum weight of the check operators. We find that for any rate beneath the capacity, high-performing codes with thousands of logical qubits are achievable with depth 4–8 expurgated random circuits in D = 2 dimensions. These results indicate that finite-rate quantum codes are practically relevant for near-term devices and may significantly reduce the resource requirements to achieve fault tolerance for near-term applications.

Additional Information

© 2021 The Author(s). Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI. (Received 13 November 2020; revised 11 June 2021; accepted 12 July 2021; published 24 September 2021) We thank Steve Girvin, Pradeep Niroula, and Sarang Gopalakrishnan for helpful discussions. M. J. G. and D. A. H. were supported in part by the Defense Advanced Research Projects Agency (DARPA) Driven and Nonequilibrium Quantum Systems (DRINQS) program. L. J. acknowledges support from the Army Research Office (ARO) (Grants No. W911NF-18-1-0020 and No. W911NF-18-1-0212), ARO MURI (Grant No. W911NF-16-1-0349), Air Force Office of Scientific Research (AFOSR) MURI (Grant No. FA9550-19-1-0399), Department of Energy (DOE) (Grant No. DE-SC0019406), National Science Foundation (NSF) (Grants No. EFMA-1640959, No. OMA-1936118, and No. EEC-1941583), and the Packard Foundation (Grant No. 2013-39273).

Attached Files

Published - PhysRevX.11.031066.pdf

Accepted Version - 2010.09775.pdf

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Additional details

Created:
August 20, 2023
Modified:
October 23, 2023