Perfect teleportation of an arbitrary three-qubit state with the highly entangled six-qubit genuine state  被引量:7

Perfect teleportation of an arbitrary three-qubit state with the highly entangled six-qubit genuine state

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作  者:YIN XiaoFeng 1,LIU YiMin 2,ZHANG ZiYun 1,ZHANG Wen 1 & ZHANG ZhanJun 1 1 Key Laboratory of Optoelectronic Information Acquisition & Manipulation of Ministry of Education of China,School of Physics & Material Science,Anhui University,Hefei 230039,China 2 Department of Physics,Shaoguan University,Shaoguan 512005,China 

出  处:《Science China(Physics,Mechanics & Astronomy)》2010年第11期2059-2063,共5页中国科学:物理学、力学、天文学(英文版)

基  金:partly supported by the program for New Century Excellent Talents at the University of China (Grant No.NCET-06-0554);the National Natural Science Foundation of China (Grant Nos.60677001,10747146 and 10874122);the Science-technology Fund of Anhui Province for Outstanding Youth (Grant No.06042087);the Key Fund of the Ministry of Education of China (Grant No.206063);the Talent Foundation of Higher Education of Anhui Province for Outstanding Youth (Grant No.2009SQRZ018);the Natural Science Foundation of Guangdong Province (Grant Nos.06300345 and 7007806)

摘  要:The perfect teleportation of an arbitrary three-qubit state with the highly entangled six-qubit genuine state introduced by Borras et al.(J.Phys.A: Math.Theor.40 (2007) 13407) is studied.Some appropriate measuring bases the sender can take and the corresponding unitary operations the receiver should execute in terms of the sender’s measurement outcome are explicitly given.The flexibility between the measurement difficulty and the reconstruction difficulty is shown.Moreover,discussions and comparisons between our scheme and the recent incomplete scheme (Choudhury et al,J.Phys.A: Math.Theor.42 (2009) 115303) are made.The perfect teleportation of an arbitrary three-qubit state with the highly entangled six-qubit genuine state introduced by Borras et al.(J.Phys.A: Math.Theor.40 (2007) 13407) is studied.Some appropriate measuring bases the sender can take and the corresponding unitary operations the receiver should execute in terms of the sender’s measurement outcome are explicitly given.The flexibility between the measurement difficulty and the reconstruction difficulty is shown.Moreover,discussions and comparisons between our scheme and the recent incomplete scheme (Choudhury et al,J.Phys.A: Math.Theor.42 (2009) 115303) are made.

关 键 词:quantum TELEPORTATION highly ENTANGLED six-qubit GENUINE STATE measuring bases reconstruction operation flexibility 

分 类 号:O413.1[理学—理论物理]

 

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