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首页> 外文期刊>PHYSICAL REVIEW A >Two-qubit mixed states more entangled than pure states: Comparison of the relative entropy of entanglement for a given nonlocality
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Two-qubit mixed states more entangled than pure states: Comparison of the relative entropy of entanglement for a given nonlocality

机译:比纯态更纠缠的两量子位混合态:给定非局部性的纠缠相对熵的比较

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摘要

Amplitude damping changes entangled pure states into usually less-entangled mixed states.We show, however,nthat even local amplitude damping of one or two qubits can result in mixed states more entangled than purenstates if one compares the relative entropy of entanglement (REE) for a given degree of the Bell–Clauser-Horne-nShimony-Holt inequality violation (referred to as nonlocality). By applying Monte Carlo simulations, we find thenmaximally entangled mixed states and showthat they are likely to be optimal by checking the Karush-Kuhn-Tuckernconditions, which generalize the method of Lagrange multipliers for this nonlinear optimization problem. Wenshow that the REE for mixed states can exceed that of pure states if the nonlocality is in the range (0,0.82) and thenmaximal difference between theseREEs is 0.4.Aformer comparison [Phys. Rev. A 78, 052308 (2008)] of theREEnfor a given negativity showed analogous property but the corresponding maximal difference in the REEs is onenorder smaller (i.e., 0.039) and the negativity range is (0,0.53) only. For appropriate comparison, we normalizednthe nonlocality measure to be equal to the standard entanglement measures, including the negativity, for arbitraryntwo-qubit pure states. We also analyze the influence of the phase-damping channel on the entanglement of theninitially pure states. We show that the minimum of the REE for a given nonlocality can be achieved by thisnchannel, contrary to the amplitude-damping channel.
机译:振幅阻尼将纠缠的纯态转变为通常纠缠程度较小的混合态。但是,我们证明,如果一个或两个量子位的局部振幅阻尼比混合态的相对熵(REE)相对于纯态,则混合态的纠缠比纯态更纠缠。给定程度的Bell–Clauser-Horne-nShimony-Holt不等式违规(称为非局部性)。通过应用蒙特卡洛模拟,我们找到了最大纠缠的混合态,并通过检查Karush-Kuhn-Tuckern条件表明它们可能是最优的,该条件将Lagrange乘子的方法推广到了该非线性优化问题。 Wenshow指出,如果非局部性在(0,0.82)范围内,则这些混合态的REE可以超过纯态的REE,然后这些REE之间的最大差为0.4。对于给定的负极性,REEn的A. Rev. A 78,052308(2008)]显示出类似的性质,但是REE中相应的最大差值依次变小(即0.039),并且负极性范围仅为(0,0.53)。为了进行适当的比较,我们将非局部性度量标准化为等于任意n个双量子位纯态的标准纠缠度,包括负性。我们还分析了相位衰减通道对最初纯态纠缠的影响。我们表明,与振幅衰减通道相反,给定非局部性的REE最小值可以通过此通道实现。

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  • 来源
    《PHYSICAL REVIEW A》 |2013年第4期|1-9|共9页
  • 作者单位

    Faculty of Physics Adam Mickiewicz University 61-614 Pozna´n Poland;

    RCPTM Joint Laboratory of Optics of Palack´y University and Institute of Physics of Academy of Sciences of the Czech Republic 17.listopadu 12 772 07 Olomouc Czech Republic;

    Faculty of Physics Adam Mickiewicz University 61-614 Pozna´n Poland;

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