Direct Purification of Bell and Multipartite GHZ States via Weak Measurement

IF 4.4 Q1 OPTICS
Sajede Harraz, Shuang Cong
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引用次数: 0

Abstract

Maximally entangled states are crucial for various quantum information processing, yet their quality suffers from entanglement loss due to decoherence. In this paper, a direct purification technique that utilizes weak measurement and requires only two copies of the entangled state is proposed. The method involves transforming the damped entangled state with weak measurements and then applying a direct purification process. This approach yields a maximally entangled state with a certain probability. In the context of Bell state purification, two weak measurement-based operations designed to convert amplitude-damped Bell states into the desired state for direct purification method are presented. The first operation is applied prior to the noisy channel, while the second is employed after the noisy channel. Through comprehensive analysis, the performances of these two schemes are evaluated and compared and benchmarked them against a pioneering weak measurement-based scheme. The findings demonstrate that the proposed methods exhibit superior performance in terms of both fidelity and probability. Additionally, a novel technique for purifying multipartite amplitude-damped Greenberger–Horne–Zeilinger (GHZ) states is introduced, which existing methods cannot address. By employing only two copies of the entangled states and harnessing the unique advantages of weak measurement operations, the method achieves both resource efficiency and effectiveness.

利用弱测量直接纯化贝尔态和多部GHZ态
最大纠缠态是各种量子信息处理的关键,但其质量受到退相干导致的纠缠损失的影响。本文提出了一种利用弱测量且只需要两个纠缠态副本的直接净化技术。该方法包括用弱测量转换阻尼纠缠态,然后应用直接净化过程。这种方法产生具有一定概率的最大纠缠态。在贝尔状态净化的背景下,提出了两种基于弱测量的操作,旨在将幅度阻尼贝尔状态转换为直接净化方法所需的状态。第一种操作在噪声信道之前应用,而第二种操作在噪声信道之后应用。通过综合分析,对这两种方案的性能进行了评价和比较,并与一种开创性的基于弱测量的方案进行了基准测试。研究结果表明,所提出的方法在保真度和概率方面都表现出优异的性能。此外,介绍了一种新的多部幅阻尼格林伯格-霍恩-塞林格(GHZ)态的净化技术,这是现有方法无法解决的问题。该方法仅使用两个纠缠态副本,利用弱测量操作的独特优势,实现了资源效率和有效性的结合。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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CiteScore
7.90
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0.00%
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