四量子比特系统的几何真正多方纠缠

Q2 Physics and Astronomy Physics Open Pub Date : 2024-08-01 DOI:10.1016/j.physo.2024.100230
Ansh Mishra , Soumik Mahanti , Abhinash Kumar Roy , Prasanta K. Panigrahi
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引用次数: 0

摘要

Xie 和 Eberly 为三方系统引入了一种真正的多方纠缠(GME)度量 "一致性填充"(concurrence fill)(Xie 和 Eberly,2021 年)。它被定义为一个三角形的面积,该三角形的边长代表每个双分区中一致度的平方。然而,最近的研究表明,在 LOCC 条件下,一致性填充不是单调的,因此不是纠缠的忠实度量。虽然它不是一个忠实的纠缠度量,但它包含了对双分区平方并合的一种优雅的几何解释。有一些人尝试将 GME 量化器推广到四方环境及其他环境。然而,其中一些并不忠实,另一些则缺乏优雅的几何解释。Xie 等人最近提出的建议构建了一个并发四面体,它的体积给出了四方系统的 GME 量;将其推广到多于四方的系统中,就是简单四面体结构在该维度上的超体积。在这里,我们通过构造证明,要捕捉多方纠缠的所有方面,并不需要更复杂的结构,只需使用二维几何就能证明四方纠缠。亚二维性与线性熵的荒木-李布不等式被用来构建几何 GME 量子的直接扩展,使其适用于四边形几何中的四方系统。我们的量子可以从几何角度解释为三个四边形的组合,其边是一比三的双分区中的并合,对角线是二比二的双分区中的并合。
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Geometric genuine multipartite entanglement for four-qubit systems

Xie and Eberly introduced a genuine multipartite entanglement (GME) measure ‘concurrence fill’ (Xie and Eberly, 2021) for three-party systems. It is defined as the area of a triangle whose side lengths represent squared concurrence in each bi-partition. However, it has been recently shown that concurrence fill is not monotonic under LOCC, hence not a faithful measure of entanglement. Though it is not a faithful entanglement measure, it encapsulates an elegant geometric interpretation of bipartite squared concurrences. There have been a few attempts to generalize GME quantifier to four-party settings and beyond. However, some of them are not faithful, and others simply lack an elegant geometric interpretation. The recent proposal from Xie et al.. constructs a concurrence tetrahedron, whose volume gives the amount of GME for four-party systems; with generalization to more than four parties being the hypervolume of the simplex structure in that dimension. Here, we show by construction that to capture all aspects of multipartite entanglement, one does not need a more complex structure, and the four-party entanglement can be demonstrated using 2D geometry only. The subadditivity together with the Araki-Lieb inequality of linear entropy is used to construct a direct extension of the geometric GME quantifier to four-party systems resulting in quadrilateral geometry. Our quantifier can be geometrically interpreted as a combination of three quadrilaterals whose sides result from the concurrence in one-to-three bi-partition, and diagonal as concurrence in two-to-two bipartition.

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来源期刊
Physics Open
Physics Open Physics and Astronomy-Physics and Astronomy (all)
CiteScore
3.20
自引率
0.00%
发文量
19
审稿时长
9 weeks
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