Compare the Pair: Rotated vs. Unrotated Surface Codes at Equal Logical Error Rates
Practical quantum computers will require resource-efficient error-correcting codes. The rotated surface code uses approximately half the number of qubits as the unrotated surface code to create a logical qubit with the same error-correcting distance. However, instead of distance, a more useful qubit...
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Zusammenfassung: | Practical quantum computers will require resource-efficient error-correcting
codes. The rotated surface code uses approximately half the number of qubits as
the unrotated surface code to create a logical qubit with the same
error-correcting distance. However, instead of distance, a more useful
qubit-saving metric would be based on logical error rates. In this work we find
the well-below-threshold scaling of logical to physical error rates under
circuit-level noise for both codes at high odd and even distances, then compare
the number of qubits used by each code to achieve equal logical error rates. We
perform Monte Carlo sampling of memory experiment circuits with all valid CNOT
orders, using the stabiliser simulator Stim and the uncorrelated minimum-weight
perfect-matching decoder PyMatching 2. We find that the rotated code uses $74 -
75\%$ the number of qubits used by the unrotated code, depending on the noise
model, to achieve a logical error rate of $p_L = 10^{-12}$ at the operational
physical error rate of $p=10^{-3}$. The ratio remains $\approx75\%$ for
physical error rates within a factor of two of $p=10^{-3}$ for all useful
logical error rates. Our work finds the low-$p_L$ scaling of the surface code
and clarifies the qubit savings provided by the rotated surface code, providing
numerical justification for its use in future implementations of the surface
code. |
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DOI: | 10.48550/arxiv.2409.14765 |