Exploring quantum properties of bipartite mixed states under coherent and incoherent basis

IF 0.7 4区 物理与天体物理 Q3 COMPUTER SCIENCE, THEORY & METHODS International Journal of Quantum Information Pub Date : 2022-06-16 DOI:10.1142/S0219749923500107
Sovik Roy, A. Bhattacharjee, C. Radhakrishnan, Md. Manirul Ali, B. Ghosh
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Abstract

Quantum coherence and quantum entanglement are two different manifestations of the superposition principle. In this article we show that the right choice of basis to be used to estimate coherence is the separable basis. The quantum coherence estimated using the Bell basis does not represent the coherence in the system, since there is a coherence in the system due to the choice of the basis states. We first compute the entanglement and quantum coherence in the two qubit mixed states prepared using the Bell states and one of the states from the computational basis. The quantum coherence is estimated using the l1-norm of coherence, the entanglement is measured using the concurrence and the mixedness is measured using the linear entropy. Then we estimate these quantities in the Bell basis and establish that coherence should be measured only in separable basis, whereas entanglement and mixedness can be measured in any basis. We then calculate the teleportation fidelity of these mixed states and find the regions where the states have a fidelity greater than the classical teleportation fidelity. We also examine the violation of the Bell-CHSH inequality to verify the quantum nonlocal correlations in the system. The estimation of the above mentioned quantum correlations, teleportation fidelity and the verification of Bell-CHSH inequality is also done for bipartite states obtained from the tripartite systems by the tracing out of one of their qubits. We find that for some of these states teleportation is possible even when the Bell-CHSH inequality is not violated, signifying that nonlocality is not a necessary condition for quantum teleportation.
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探讨二部混合态在相干和非相干基下的量子性质
量子相干和量子纠缠是叠加原理的两种不同表现形式。在本文中,我们证明了用于估计相干性的基的正确选择是可分离基。使用Bell基估计的量子相干性并不代表系统中的相干性,因为由于基态的选择,系统中存在相干性。我们首先从计算基础上计算使用Bell态和其中一个态制备的两个量子位混合态中的纠缠和量子相干。量子相干是使用相干的l1范数来估计的,纠缠是使用并发性来测量的,混合性是使用线性熵来测量的。然后,我们在Bell基中估计这些量,并确定相干只能在可分离基中测量,而纠缠和混合性可以在任何基中测量。然后,我们计算这些混合态的隐形传态保真度,并找到这些态的保真度大于经典隐形传态逼真度的区域。我们还检验了Bell-CHSH不等式的违反,以验证系统中的量子非局部相关性。对于通过追踪三方系统中的一个量子位获得的二分态,还对上述量子相关性、隐形传态保真度和Bell-CHS不等式的验证进行了估计。我们发现,对于其中一些状态,即使不违反Bell-CHS不等式,隐形传态也是可能的,这意味着非局域性不是量子隐形传态的必要条件。
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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来源期刊
International Journal of Quantum Information
International Journal of Quantum Information 物理-计算机:理论方法
CiteScore
2.20
自引率
8.30%
发文量
36
审稿时长
10 months
期刊介绍: The International Journal of Quantum Information (IJQI) provides a forum for the interdisciplinary field of Quantum Information Science. In particular, we welcome contributions in these areas of experimental and theoretical research: Quantum Cryptography Quantum Computation Quantum Communication Fundamentals of Quantum Mechanics Authors are welcome to submit quality research and review papers as well as short correspondences in both theoretical and experimental areas. Submitted articles will be refereed prior to acceptance for publication in the Journal.
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