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理论物理通讯:英文版

Controlled Quantum Teleportation Through Noisy GHZ Channel

苗纯, 杨名, 曹卓良

Published Jan 1, 2010• 0 citations
OpenAlex

Abstract

在这份报纸,我们为 teleporting 建议二个物理计划通过在洞证完的吵闹的隧道的一个未知原子状态。量隧道是吵闹的混合 GHZ 说,它在量信息处理是更现实主义的。我们解决经分解在 Lindblad 形式与的一个主人方程(L2, z, L3, z, L4, z ) 在洞证完的噪音的类型。在二个协议之间的比较被讨论。

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Which state loses less quantum information between Greenberger-Horne-Zeilinger (GHZ) and $W$ states when they are prepared for two-party quantum teleportation through a noisy channel? We address this issue by solving analytically a master equation in the Lindblad form with introducing the noisy channels that cause the quantum channels to be mixed states. It is found that the answer to this question is dependent on the type of noisy channel. If, for example, the noisy channel is $({L}_{2,x},{L}_{3,x},{L}_{4,x})$ type, where the $L$'s denote the Lindblad operators, the GHZ state is always more robust than the $W$ state, i.e., the GHZ state preserves more quantum information. In, however, the $({L}_{2,y},{L}_{3,y},{L}_{4,y})$-type channel the situation becomes completely reversed. In the $({L}_{2,z},{L}_{3,z},{L}_{4,z})$-type channel, the $W$ state is more robust than the GHZ state when the noisy parameter $(\ensuremath{\kappa})$ is comparatively small while the GHZ state becomes more robust when $\ensuremath{\kappa}$ is large. In isotropic noisy channel we found that both states preserve an equal amount of quantum information. A relation between the average fidelity and entanglement for the mixed state quantum channels are discussed.

arXiv:0801.1433•Physical Review A•Jul 9, 2008•137 citations
在这份报纸,我们为 teleporting 建议二个物理计划通过在洞证完的吵闹的隧道的一个未知原子状态。量隧道是吵闹的混合 GHZ 说,它在量信息处理是更现实主义的。我们解决经分解在 Lindblad 形式与的一个主人方程(L2, z, L3, z, L4, z ) 在洞证完的噪音的类型。在二个协议之间的比较被讨论。
Which state loses less quantum information between Greenberger-Horne-Zeilinger (GHZ) and WWW states when they are prepared for two-party quantum teleportation through a noisy channel? We address this issue by solving analytically a master equation in the Lindblad form with introducing the noisy channels that cause the quantum channels to be mixed states. It is found that the answer to this question is dependent on the type of noisy channel. If, for example, the noisy channel is (L2,x,L3,x,L4,x)({L}_{2,x},{L}_{3,x},{L}_{4,x})(L2,x​,L3,x​,L4,x​) type, where the LLL's denote the Lindblad operators, the GHZ state is always more robust than the WWW state, i.e., the GHZ state preserves more quantum information. In, however, the (L2,y,L3,y,L4,y)({L}_{2,y},{L}_{3,y},{L}_{4,y})(L2,y​,L3,y​,L4,y​)-type channel the situation becomes completely reversed. In the (L2,z,L3,z,L4,z)({L}_{2,z},{L}_{3,z},{L}_{4,z})(L2,z​,L3,z​,L4,z​)-type channel, the WWW state is more robust than the GHZ state when the noisy parameter $(\ensuremath{\kappa})$ is comparatively small while the GHZ state becomes more robust when $\ensuremath{\kappa}$ is large. In isotropic noisy channel we found that both states preserve an equal amount of quantum information. A relation between the average fidelity and entanglement for the mixed state quantum channels are discussed.