| 借助于推广Bell态实现两体量子态隐形传态 |
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| 引用本文： | 曹海静,陈中华,朱燕艳,宋鹤山.借助于推广Bell态实现两体量子态隐形传态[J].大连理工大学学报,2010,50(4):469-474. |
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| 作者姓名： | 曹海静 陈中华 朱燕艳 宋鹤山 |
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| 作者单位： | 1. 上海电力学院,直属教理系,上海,201300
2. 大连理工大学,物理与光电工程学院,辽宁,大连,116024 |
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| 基金项目： | 国家自然科学基金资助项目，上海市教委创新基金资助项目，上海市高校杰出青年教师科研基金资助项目 |
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| 摘 要： | 两比特量子隐形传态的实现直接关系到量子计算机的实现,因此提出一个任意两比特量子态的隐形传态方案,发送者能成功地将此量子态几率地传送给接收者.此方案中,16个推广的非最大纠缠Bell态(简称G态)之一充当量子信道.发送者通过实行推广的Bell态测量(G态测量),接收者通过引入一个辅助粒子并实施适当的么正变换和单粒子测量,能将此任意两比特量子态以一定的几率发送给接收者.此种隐形传态方案的成功几率由量子信道系数绝对值的最小值所决定.Abstract：Two-qubit quantum teleportation is closely related to quantum computation, so a teleportation protocol in which an arbitrary bipartite quantum state is perfectly teleported probabilistically from sender to receiver is proposed. One of 16 generalized non-maximally entangled Bell states (G states for simplicity) functions as quantum channel. The teleportation can be successfully realized with a certain probability if sender performs generalized Bell state measurements (G measurements) and receiver introduces an auxiliary particle and operates appropriate unitary transformations and single-qubit measurements. The probability of successful teleportation is determined by the smallest one among the coefficients' absolute values of the quantum channel.
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| 关 键 词： | 隐形传态 推广Bell态 辅助粒子 么正变换 |
Teleportation of a bipartite quantum state via generalized Bell states |
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| CAO Haijing,CHEN Zhonghu,ZHU Yanyan,SONG Heshan.Teleportation of a bipartite quantum state via generalized Bell states[J].Journal of Dalian University of Technology,2010,50(4):469-474. |
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| Authors: | CAO Haijing CHEN Zhonghu ZHU Yanyan SONG Heshan |
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| Institution: | CAO Hai-jing1,CHEN Zhong-hua1,ZHU Yan-yan1,SONG He-shan21.Physics Department,Shanghai University of Electric Power,Shanghai 201300,China,2.School of Physics and Optoelectronic Engineering,Dalian University of Technology,Dalian 116024 |
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| Abstract: | Two-qubit quantum teleportation is closely related to quantum computation, so a teleportation protocol in which an arbitrary bipartite quantum state is perfectly teleported probabilistically from sender to receiver is proposed. One of 16 generalized non-maximally entangled Bell states (G states for simplicity) functions as quantum channel. The teleportation can be successfully realized with a certain probability if sender performs generalized Bell state measurements (G measurements) and receiver introduces an auxiliary particle and operates appropriate unitary transformations and single-qubit measurements. The probability of successful teleportation is determined by the smallest one among the coefficients' absolute values of the quantum channel. |
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| Keywords: | teleportation generalized Bell states auxiliary particle unitary transformations |
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