Abstract

We numerically study coherent errors in surface codes on planar graphs, focusing on noise of the form of $Z$- or $X$-rotations of individual qubits. We find that, similarly to the case of incoherent bit- and phase-flips, a trade-off between resilience against coherent $X$- and $Z$-rotations can be made via the connectivity of the graph. However, our results indicate that, unlike in the incoherent case, the error-correction thresholds for the various graphs do not approach a universal bound. We also study the distribution of final states after error correction. We show that graphs fall into three distinct classes, each resulting in qualitatively distinct final-state distributions. In particular, we show that a graph class exists where the logical-level noise exhibits a decoherence threshold slightly above the error-correction threshold. In these classes, therefore, the logical level noise above the error-correction threshold can retain significant amount of coherence even for large-distance codes. To perform our analysis, we develop a Majorana-fermion representation of planar-graph surface codes and describe the characterization of logical-state storage using fermion-linear-optics-based simulations. We thereby generalize the approach introduced for the square lattice by Bravyi \textit{et al}. [npj Quantum Inf. 4, 55 (2018)] to surface codes on general planar graphs.

Highlights

  • In recent years, significant progress has been made to improve the coherence times of qubits [1,2,3], including demonstrations of key ingredients for quantum error correction (QEC) [4,5,6,7,8]

  • We described how the C4 encoding of qubits can be used to obtain a Majorana-fermion representation of surface codes on arbitrary planar graphs, and we characterized logical-state storage under coherent Z rotations using fermion linear optics (FLO)-based simulations

  • Comparing ηth to the thresholds ηtPh for the Pauli twirl of the physical-qubit coherent error, we found that while ηth and ηtPh are similar, the inequality ηth ηtPh holds for all considered systems

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Summary

INTRODUCTION

Significant progress has been made to improve the coherence times of qubits [1,2,3], including demonstrations of key ingredients for quantum error correction (QEC) [4,5,6,7,8]. The size of the system was not sufficient to establish a threshold but it provided evidence that using the so-called Pauli twirl to approximate coherent errors as incoherent noise on the level of physical qubits underestimates the logical error rate. We describe a general approach for representing surface codes with Majorana fermions on arbitrary planar graphs, including planar lattices, and show how the FLO-based algorithm can be adapted to this case For incoherent errors, it was found [31,32] that by changing the lattice geometry, one can trade off resilience against phase flips for resilience against bit flips. En route to our analysis of the logical-level coherence, we describe a coherent decoder that takes advantage of the deterministic nature of coherent errors

SURFACE CODE ON GENERAL LATTICES
ERROR MODELS
QUANTUM ERROR-CORRECTION AND ITS CHARACTERIZATION
MAJORANA GRAPH
FLO SIMULATION
AVERAGE LOGICAL CHANNEL
VIII. THRESHOLD
FINAL-STATE DISTRIBUTION
NOISE DECOHERENCE THRESHOLDS AND THE COHERENT DECODER
CONCLUSION
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