共查询到18条相似文献,搜索用时 62 毫秒
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利用一个(N 1)粒子部分纠缠Greenberger-Home-Zeilinger(GHZ)态作为量子通道,提出了概率远程制备N粒子GHZ态的两个方案.我们考虑了怎样远程制备一个任意的GHZ态,即两个参数α和β都是复数的情况.此外,计算了远程制备总的成功概率和需要的经典信息量. 相似文献
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提出了利用部分纠缠的特殊二粒子W态和部分纠缠的二粒子态组成量子信道,隐形传送一个二粒子纠缠态的方案。发送者进行两次Bell基测量,接受者先在{|0〉,|1〉}基下进行一次测量,然后实施一次控制—非操作,最后引进一个辅助粒子并进行一组适当的幺正变换操作,便可以一定的概率实现二粒子纠缠态的隐形传送。分析表明:当量子信道处于最大纠缠,即信道由一个特殊二粒子W态和一个Bell态组成时,本方案的传输概率达到2/3,传输效果介于完全由W态组成量子信道与完全由Bell态组成量子信道的方案之间。 相似文献
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利用非Bell基测量实现两粒子纠缠态的隐形传输 总被引:2,自引:1,他引:1
研究无Bell基测量的未知两粒子纠缠态的隐形传态方案。Alice需传送未知两原子纠缠态给Bob,以她和Bob的原子组成的最大纠缠GHZ态作为量子信道,通过两原子同时在一个强经典驱动场驱动下和一个单模腔场发生相互作用,产生态的演化,从而实现隐形传态。本方案可忽略腔场热作用和腔延迟作用的影响,传送成功的总几率为1。 相似文献
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远程制备双原子纠缠态 总被引:1,自引:1,他引:0
提出一种远程制备双原子纠缠态的方案,该方案基于两个原子与单模腔场的同时非共振相互作用.由于双粒子纠缠态比三粒子纠缠态容易制备,方案用两对双原子纠缠态作为量子通道.Alice 拥有的两个相同原子同时与一单模腔场非共振相互作用.Alice已知她要制备的纠缠态,她选择适当的相互作用时间、测量她所拥有的两个原子并通过经典通道通知Bob.Bob引入一个相同的辅助原子和一个单模腔场来实现方案.方案对腔场状态和腔损耗不敏感,基于当前的腔QED 技术,方案能在实验上实现.该方案有望在量子信息过程中有重要的应用价值. 相似文献
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远程制备多粒子纯态 总被引:2,自引:1,他引:1
我们提出了一个远程制备三种形式的多粒子纯态的方案,远程制备一般形式的多粒子纯态及两种特殊情况下的多粒子纯态.首先利用大失谐腔制备出N个原子的纠缠态[14],并将这N个原子分配给Alice和Bob等其他的参与者.然后Alice根据要远程制备的态对她的原子进行相应的单原子投影测量,并且将测量结果以经典信息的方式告诉给其他参与者.其他参与者根据收到的信息决定对自己的原子要么不操作,要么进行特定的操作,来转换他们所共享的纠缠态,最终除Alice以外的参与者就会处于期望的纠缠态.每一种情况下的信息消耗都是很少的,只消耗一量子比特和一经典比特.整个方案都基于现有的腔量子电动力学技术,因此该方案是可行性的. 相似文献
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四粒子纠缠的一般W态的退纠缠和W态的概率隐形传态 总被引:5,自引:2,他引:3
我们推广地得到了到四粒子纠缠的一般W态,给出了一般W态的不同退纠缠的条件,得到了一个新的二粒子的一般W态,并得到对于四粒子纠缠的一般W态而言,其系数α1,α2和α3从一个直到全部为零时,这一般的|ΨW〉依次有一个粒子,二个粒子和最后全部粒子退出纠缠。还给出了一个利用四个二粒子纠缠态作为量子信道来传送四粒子纠缠W态的方案,并且进一步给出了当量子信道为非最大纠缠态时,四粒子纠缠的一般W态的隐形传态的一个方案,同时通过构造一个5×5对角投影变换矩阵,解决了使用一般纠缠量子信道并不再引入辅助态时,态畸变的恢复问题.并且这里的对角投影变换UM也与以往文献中的不同,而且比过去文献的讨论更直接.因本文的研究是一般性的,本文关于对角的投影变换矩阵UM的变换方法等可以直接推广到任意一般纠缠信道的一般纠缠态的概率隐形传态。 相似文献
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We present a protocol for probabilistic remote preparation of the two-atom maximally entangled state using a four-atom GHZ
entangled state as the quantum channel. The two-atom maximally entangled state can be successfully prepared between two distant
parties with a success probability of 100%. The successful total probability and classical communication cost are calculated. 相似文献
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We propose a protocol where one can realize quantum cloning of an unknown two-particle entangled state and its orthogonal-complement
state with assistance offered by a state preparer. The first stage of the protocol requires usual teleportation using a (or
two) four-particle entangled state(s) as quantum channel(s). In the second stage of the protocol, with the assistance (through
a two-particle projective measurement) of the preparer, the perfect copies and complement copies of an unknown state can be
produced. 相似文献
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SHI Jin ZHAN You-Bang 《理论物理通讯》2009,51(2):239-243
We present a scheme for probabilistic remote preparation of a tripartite qutrit entangled state with a partial tripartite qutrit entangled state and a partial bipartite qutrit entangled state as the quantum channel. It is found that a bipartite qutrit orthogonal projective measurement, an auxiliary qutrit particle, and the corresponding unitary transformation are required. A scheme for probabilistic remote preparation of a tripartite qudit equatorial entangled state by using a partial tripartite qudit entangled state and a partial bipartite qudit entangled state as the quantum channel is also proposed. We calculate the successful total probability and the total classical communication cost required in the RSP process, respectively. 相似文献
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JIANG Wei-Xing FANG Jian-Xing ZHU Shi-Qun SHA Jin-Qiao 《理论物理通讯》2007,47(6):1045-1048
A scheme for controlled teleportation of an unknown N-qubit entangled GHZ state from the sender Alice to the distant receiver Bob is proposed. And m-qubit GHZ state is sufficient for the task of control by m spatially- separated supervisors. Conditioned on the local operations executed by all participants, Bob can faithfully restore the original state by performing relevant unitary transformations with the aid of some classical message about measurement results. Anyone's absence will absolutely lead to the failure of teleportation. 相似文献
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We propose a scheme for multiparty-controlled remote preparation of the two-particle state by using two non-maximally Greenberger-Horne-Zeilinger states as quantum channel. Our scheme consists of one sender and n remote receivers. It will be shown that the sender can help either one of the n receivers to remotely preparation the original state with the appropriate probability, and the sender Alice's two-particle projective measurement and the controllers' single-particle product meazurements are needed. We also obtained the probability of the successful remote state preparation. 相似文献
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In this scheme, N non-maximally entangled particle pairs are used as quantum channel to teleport an unknown N-particle entangled GHZ state via entanglement swapping. In order to realize this teleportation, the sender Alice operates Bell-state measurement on particles belonging to herself. Then she informs the results to the receiver Bob through classical communication. According to the results, Bob operates corresponding transformation to reconstruct the initial state. The advantage of this scheme is that it needs only one common unitary matrix for Alice‘s different results, which has a more general meaning. As a special case, teleporting an unknown three-particle entangled GHZ state is proposed. 相似文献