论文标题

局部近似,以完美歧视量子状态

Local approximation for perfect discrimination of quantum states

论文作者

Cohen, Scott M.

论文摘要

量子状态歧视涉及从一组可能的状态中识别给定状态。当国家是相互正交的时,使用全球测量始终可以进行完美的状态歧视。在各方限制使用多个回合的本地操作和经典交流(LOCC)的情况下,即使使用\ emph {渐近locc},通常不可能使用多个回合的状态歧视,但在其中允许错误,但必须消失在无限次数的限制中。利用我们在渐近LOCC上的最新结果,我们在LOCC歧视任何给定的一组相互正交纯状态的误差概率上得出了一个下限。在从这个下限中获得的见解得出的信息,我们能够证明通过渐近LOCC进行完美的国家歧视所必需的条件。然后,我们以示例说明这些必要条件在显着简化是否可以使用LOCC任意密切完成对给定状态的完美歧视的确定中的能力。后一个示例包括一个证据表明,对于某个\ emph {minimal}不可扩展的产品碱(UPB)的某个子集的完美歧视是不可能的,其中最小意味着对于给定的多部分系统,没有较小状态的UPB可以存在。我们还提供了一个简单的证据,表明所谓的\ emph {没有纠缠的强非局部性}比以前证明的要强得多。

Quantum state discrimination involves identifying a given state out of a set of possible states. When the states are mutually orthogonal, perfect state discrimination is always possible using a global measurement. In the case of multipartite systems when the parties are constrained to use multiple rounds of local operations and classical communication (LOCC), perfect state discrimination is often impossible even with the use of \emph{asymptotic LOCC}, wherein an error is allowed but must vanish in the limit of an infinite number of rounds. Utilizing our recent results on asymptotic LOCC, we derive a lower bound on the error probability for LOCC discrimination of any given set of mutually orthogonal pure states. Informed by the insights gained from this lower bound, we are able to prove necessary conditions for perfect state discrimination by asymptotic LOCC. We then illustrate by example the power of these necessary conditions in significantly simplifying the determination of whether perfect discrimination of a given set of states can be accomplished arbitrarily closely using LOCC. The latter examples include a proof that perfect discrimination by asymptotic LOCC is impossible for a certain subset of \emph{minimal} unextendible product bases (UPB), where minimal means that for the given multipartite system, no UPB with a smaller number of states can exist. We also give a simple proof that what has been called \emph{strong nonlocality without entanglement} is considerably stronger than had previously been demonstrated.

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