J4 ›› 2010, Vol. 27 ›› Issue (2): 167-173.

• 量子光学 • 上一篇    下一篇

利用cluster态实现任意两粒子纠缠态的概率隐形传态 的量子概率隐形传态*

于立志1,吴幍2   

  1. 1. 阜阳师范学院
    2.
  • 收稿日期:2009-06-08 修回日期:2010-03-05 出版日期:2010-03-28 发布日期:2010-03-05
  • 通讯作者: 于立志

Probabilistic Teleportation of Arbitrary Two-Particle Entangled State via Cluster tate

  • Received:2009-06-08 Revised:2010-03-05 Published:2010-03-28 Online:2010-03-05

摘要: 提出两个概率隐形传态方案,这两个方案都是以一个四粒子cluster非最大纠缠态作为量子信道来实现未知两粒子纠缠态的隐形传态。在第一个方案中我们传送的是一个特殊的两粒子纠缠态,此纠缠态可以实现一定的概率传输,此概率由cluster态中绝对值较小的两个系数决定。在第二个方案中,我们要传送的是任意两粒子纠缠态,与第一方案相比,Bob除了需要实施幺正变换外,还要实施量子控制相位门才能重建被传送的纠缠态。与文献[Li D C, Cao Z L. Commun. Theor. Phys., 2007, 47:464]相比,我们使用的是cluster非最大纠缠态作为量子信道,因此我们的方案可以节约更多的纠缠资源和经典信息。

关键词: 量子概率隐形传态, cluster 态, Bell态测量, 幺正变换, 量子控制相位门, probabilisticquantum teleportation, cluster state, Bell state measurement, unitary transformation, quantum controlled phase gate

Abstract: Two schemes for teleporting an unknown two-particle entangled state via a four-qubit non-maximally entangled cluster state as quantum channel are proposed. In the first scheme, we teleported a special bipartite entangled state, the receiver Bob can reconstruct the original state with a certain probability according to the sender Alice’s measurement results, and the successful probability is determined by the smallest two coefficients’ absolute values of the cluster state. In the latter scheme we teleported an arbitrary two-particle entangled state. Contrast to the first scheme, Bob should perform a quantum controlled phase gate operation besides the unitary transformation. The considerable advantage of our schemes is that we employ a non-maximally entangled cluster state as quantum channel in these two schemes, which differs from the paper [Li D C, Cao Z L. Commun. Theor. Phys., 2007, 47:464]. Thus, our schemes can greatly reduce the amount of entanglement resources and need less classical bits.