论文标题
三维表面代码中的非Pauli错误
Non-Pauli Errors in the Three-Dimensional Surface Code
论文作者
论文摘要
稳定器错误纠正代码的一个强大功能是,稳定器测量将任意错误投射到Pauli错误,从而大大简化了物理错误校正过程以及代码性能的经典模拟。但是,逻辑非克利福德操作可以将Pauli错误映射到非Pauli(Clifford)错误,尽管随后的稳定器测量结果将把Clifford错误归还给Pauli错误,但所得分布将具有额外的相关性,这些相关性均取决于逻辑操作的性质和代码的结构。先前的工作研究了这些效果时,将横向$ t $门应用于三维颜色代码,并表明在相交误差的膜之间存在非本地“链接电荷”现象。在这项工作中,我们将这些结果推广到三维表面代码中的$ ccz $门的情况下,发现问题的许多方面在这种情况下更容易理解。特别是,连接电荷的出现是局部效应,而不是非本地效应。我们在此设置中使用Clifford错误的相对简单性来模拟它们对单次魔术状态准备过程的性能的影响(第一个这样的模拟是为了解释这些错误的全部效果),并发现它们对阈值的影响很大程度上取决于$ x $错误在GATE施加之前,在最新的稳定器测量之后,就会发生$ X $错误的概率。
A powerful feature of stabiliser error correcting codes is the fact that stabiliser measurement projects arbitrary errors to Pauli errors, greatly simplifying the physical error correction process as well as classical simulations of code performance. However, logical non-Clifford operations can map Pauli errors to non-Pauli (Clifford) errors, and while subsequent stabiliser measurements will project the Clifford errors back to Pauli errors the resulting distributions will possess additional correlations that depend on both the nature of the logical operation and the structure of the code. Previous work has studied these effects when applying a transversal $T$ gate to the three-dimensional colour code and shown the existence of a non-local "linking charge" phenomenon between membranes of intersecting errors. In this work we generalise these results to the case of a $CCZ$ gate in the three-dimensional surface code and find that many aspects of the problem are much more easily understood in this setting. In particular, the emergence of linking charge is a local effect rather than a non-local one. We use the relative simplicity of Clifford errors in this setting to simulate their effect on the performance of a single-shot magic state preparation process (the first such simulation to account for the full effect of these errors) and find that their effect on the threshold is largely determined by probability of $X$ errors occurring immediately prior to the application of the gate, after the most recent stabiliser measurement.