通过标记权重优化改进容错彩色编码量子计算的阈值

Yugo Takada, Keisuke Fujii
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引用次数: 0

摘要

色码是一种很有前途的量子纠错码(QEC),因为与表面码相比,色码的优势在于所有克利福德门都可以横向实现。然而,彩色编码在电路级噪声下的阈值相对较低,这主要是因为对其高重量稳定器发生器的测量会导致电路深度增加,从而引入大量误差。这使得色码不是容错量子计算的最佳候选方案。在此,我们提出了一种方法,通过使用以标志量子比特测量结果为条件的条件错误概率来优化解码器的权重,从而抑制此类错误的影响。在数值模拟中,我们通过使用整数编程解码器计算,将电路级噪声下 (4.8.8) 颜色编码的阈值从 0.14% 提高到 0.27% 左右。此外,在(6.6.6)色码中,我们实现了约 0.36% 的电路级阈值,这与之前采用相同噪声模型的研究中的最高值几乎相同。在这两种情况下,与使用单个 ancilla qubit 进行每个稳定器测量的传统方法相比,有效码距也得到了改善。因此,在物理误差率较低的情况下,实现的逻辑误差率几乎比具有相同码距的传统方法低一个数量级。即使与具有更高码距的单安其拉方法相比,考虑到我们方法中使用的量子比特数量增加,我们在大多数情况下也能实现更低的逻辑误差率。这种方法也可以应用于其他基于权重的解码器,从而使彩色编码更有希望成为 QEC 实验实施的候选方案。此外,我们还可以利用这种方法来改进更广泛类别的 QEC 码,如高速率量子低密度奇偶校验码。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

Improving Threshold for Fault-Tolerant Color-Code Quantum Computing by Flagged Weight Optimization

Improving Threshold for Fault-Tolerant Color-Code Quantum Computing by Flagged Weight Optimization
Color codes are promising quantum error-correction (QEC) codes because they have an advantage over surface codes in that all Clifford gates can be implemented transversally. However, the thresholds of color codes under circuit-level noise are relatively low, mainly because measurements of their high-weight stabilizer generators cause an increase in the circuit depth and, thus, substantial errors are introduced. This makes color codes not the best candidate for fault-tolerant quantum computing. Here, we propose a method to suppress the impact of such errors by optimizing weights of decoders using conditional error probabilities conditioned on the measurement outcomes of flag qubits. In numerical simulations, we improve the threshold of the (4.8.8) color code under circuit-level noise from 0.14% to around 0.27%, which is calculated by using an integer programming decoder. Furthermore, in the (6.6.6) color code, we achieve a circuit-level threshold of around 0.36%, which is almost the same value as the highest value in the previous studies employing the same noise model. In both cases, the effective code distance is also improved compared to a conventional method that uses a single ancilla qubit for each stabilizer measurement. Thereby, the achieved logical error rates at low physical error rates are almost one order of magnitude lower than those of the conventional method with the same code distance. Even when compared to the single-ancilla method with a higher code distance, considering the increased number of qubits used in our method, we achieve lower logical error rates in most cases. This method can also be applied to other weight-based decoders, making the color codes more promising as candidates for the experimental implementation of QEC. Furthermore, one can utilize this approach to improve a threshold of wider classes of QEC codes, such as high-rate quantum low-density parity-check codes.
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