Controller-decoder system requirements derived by implementing Shor's algorithm with surface code
Quantum Error Correction (QEC) is widely regarded as the most promising path towards quantum advantage, with significant advances in QEC codes, decoding algorithms, and physical implementations. The success of QEC relies on achieving quantum gate fidelities below the error threshold of the QEC code,...
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Zusammenfassung: | Quantum Error Correction (QEC) is widely regarded as the most promising path
towards quantum advantage, with significant advances in QEC codes, decoding
algorithms, and physical implementations. The success of QEC relies on
achieving quantum gate fidelities below the error threshold of the QEC code,
while accurately decoding errors through classical processing of the QEC
stabilizer measurements. In this paper, we uncover the critical system-level
requirements from a controller-decoder system (CDS) necessary to successfully
execute the next milestone in QEC, a non-Clifford circuit. Using a
representative non-Clifford circuit, of Shor factorization algorithm for the
number 21, we convert the logical-level circuit to a QEC surface code circuit
and finally to the physical level circuit. By taking into account all realistic
implementation aspects using typical superconducting qubit processor
parameters, we reveal a broad range of core requirements from any CDS aimed at
performing error corrected quantum computation. Our findings indicate that the
controller-decoder closed-loop latency must remain within tens of microseconds,
achievable through parallelizing decoding tasks and ensuring fast communication
between decoders and the controller. Additionally, by extending existing
simulation techniques, we simulate the complete fault-tolerant factorization
circuit at the physical level, demonstrating that near-term hardware
performance, such as a physical error rate of 0.1% and 1000 qubits, are
sufficient for the successful execution of the circuit. These results are
general to any non-Clifford QEC circuit of the same scale, providing a
comprehensive overview of the classical components necessary for the
experimental realization of non-Clifford circuits with QEC. |
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DOI: | 10.48550/arxiv.2412.00289 |