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Teleportation of two-atom entangled state in resonant cavity quantum electrodynamics

机译:共振腔量子电动力学中两个原子纠缠态的隐形传态

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摘要

An alternative scheme is presented for teleportation of a two-atom entangled state in cavity quantum electrodynamics (QED). It is based on the resonant atom-cavity field interaction. In the scheme, only one cavity is involved, and the number of the atoms needed to be detected is decreased compared with the previous scheme. Since the resonant atom-cavity field interaction greatly reduces the interaction time, the decoherence effect can be effectively suppressed during the teleportation process. The experimental feasibility of the scheme is discussed. The scheme can easily be generalized to the teleportation of N-atom Greeninger-Horne-Zeilinger (GHZ) entangled states. The number of atoms needed to be detected does not increase as the number of the atoms in the GHZ state increases.
机译:提出了一种替代方案,用于在腔量子电动力学(QED)中传送两个原子的纠缠态。它基于共振原子-空穴场的相互作用。在该方案中,仅涉及一个空腔,与先前的方案相比,需要检测的原子数减少了。由于共振原子-空穴场的相互作用大大减少了相互作用时间,因此在瞬态传输过程中可以有效地抑制退相干效应。讨论了该方案的实验可行性。该方案可以很容易地推广到N原子Greeninger-Horne-Zeilinger(GHZ)纠缠态的隐形传态。随着GHZ状态的原子数增加,需要检测的原子数不会增加。

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