arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 2005.11169quant-ph
收藏

量子多体掩蔽与量子纠错码

Quantum multipartite maskers vs quantum error-correcting codes

Kanyuan Han, Zhihua Guo, Huaixin Cao, Yuxing Du, Chuan Yang

摘要:

自从Modi等人在[PRL 120,230501(2018)]中引入了量子信息的掩蔽以来,已经发表了许多关于这个主题的讨论。本文研究了量子多体掩蔽码与量子纠错码之间的关系。我们说系统$K$的纯态的子集$Q$可以被算子$S$屏蔽到多部系统$\H^{(n)}$中,如果$Q$中的状态$|ψ\>$的所有像态$S|ψ\>$在每个子系统上具有相同的边缘状态。我们将这样的$S$称为$Q$的QMM。通过建立一个QMM的表达式,我们得到了一个QMM和QECC之间的关系,这表明等距是一个系统的所有纯态的QMM当且仅当它的范围是任何一个单擦除通道的QECC。作为应用,我们证明了不存在从$\C^2$到$\C^2\otimes\C^2\otimes\C^2$的等距万有掩蔽子,从而$\C^3$的态不能等距掩蔽到$\C^2\otimes\C^2\otimes\C^2$中.这完善了主要结果,并对[PRA 98,062306(2018)]中的一个开放问题给出了否定答案。另一个应用是$\C^d$的任意量子态可以完全隐藏在三分系统$\C^{d+1}\otimes\C^{d+1}\otimes\C^{d+1}$的任何两个子系统之间的相关性中,而任意量子态不能完全隐藏在二分系统的子系统之间的相关性中[PRL 98,080502(2007)]。

英文摘要:

Since masking of quantum information was introduced by Modi et al. in [PRL 120, 230501 (2018)], many discussions on this topic have been published. In this paper, we consider relationship between quantum multipartite maskers (QMMs) and quantum error-correcting codes (QECCs). We say that a subset $Q$ of pure states of a system $K$ can be masked by an operator $S$ into a multipartite system $\H^{(n)}$ if all of the image states $S|ψ\>$ of states $|ψ\>$ in $Q$ have the same marginal states on each subsystem. We call such an $S$ a QMM of $Q$. By establishing an expression of a QMM, we obtain a relationship between QMMs and QECCs, which reads that an isometry is a QMM of all pure states of a system if and only if its range is a QECC of any one-erasure channel. As an application, we prove that there is no an isometric universal masker from $\C^2$ into $\C^2\otimes\C^2\otimes\C^2$ and then the states of $\C^3$ can not be masked isometrically into $\C^2\otimes\C^2\otimes\C^2$. This gives a consummation to a main result and leads to a negative answer to an open question in [PRA 98, 062306 (2018)]. Another application is that arbitrary quantum states of $\C^d$ can be completely hidden in correlations between any two subsystems of the tripartite system $\C^{d+1}\otimes\C^{d+1}\otimes\C^{d+1}$, while arbitrary quantum states cannot be completely hidden in the correlations between subsystems of a bipartite system [PRL 98, 080502 (2007)].

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

↑