论文标题
无法区分的粒子系统中的纠缠
Entanglement in indistinguishable particle systems
论文作者
论文摘要
对于由可区分粒子组成的系统,存在一个商定的纠缠概念,从根本上讲,基于单独解决每个组成方的可能性。取而代之的是,相同粒子的不可区分性阻碍了他们的个人地址性,并促使了纠缠的多样化,有时不一致的定义。在本综述中,我们对相关现有方法进行了比较分析,该方法基于双方纠缠的表征,根据相关函数的行为。这样的观点提供了一个相当普遍的环境,可以在其中讨论非本地效应的存在。它是根据以下一般一致性标准执行的:i)纠缠对应于非局部相关性,无法通过本地操作产生; ii)当通过“冻结”合适的自由度“冻结”时,可以有效区分相同的颗粒时,它们的纠缠必须减少到可区分颗粒的颗粒中; iii)在没有其他量子资源的情况下,只有纠缠才能胜过经典信息协议。这三个请求提供了一个设置,可以评估现有方法的优势和劣势,以使粒子纠缠不可分,并为当前对这种关键问题的理解做出贡献。实际上,它们可以分为五个不同的类别:四个在粒子的概念上,一个基于物理模式的概念。我们表明,只有后一种方法与所有三个标准一致,其他每个标准确实违反了其中的至少一个。
For systems consisting of distinguishable particles, there exists an agreed upon notion of entanglement which is fundamentally based on the possibility of addressing individually each one of the constituent parties. Instead, the indistinguishability of identical particles hinders their individual addressability and has prompted diverse, sometimes discordant definitions of entanglement. In the present review, we provide a comparative analysis of the relevant existing approaches, which is based on the characterization of bipartite entanglement in terms of the behaviour of correlation functions. Such a a point of view provides a fairly general setting where to discuss the presence of non-local effects; it is performed in the light of the following general consistency criteria: i) entanglement corresponds to non-local correlations and cannot be generated by local operations; ii) when, by "freezing" suitable degrees of freedom, identical particles can be effectively distinguished, their entanglement must reduce to the one that holds for distinguishable particles; iii) in absence of other quantum resources, only entanglement can outperform classical information protocols. These three requests provide a setting that allows to evaluate strengths and weaknesses of the existing approaches to indistinguishable particle entanglement and to contribute to the current understanding of such a crucial issue. Indeed, they can be classified into five different classes: four hinging on the notion of particle and one based on that of physical modes. We show that only the latter approach is consistent with all three criteria, each of the others indeed violating at least one of them.