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本文提出了一个方案:将三粒子纠缠态从一个发送者传给两个接收者之一,并将其推广到N粒子纠缠态的传送。这里,我们仅用两粒子纠缠对作通道就实现了N粒子纠缠态的传送。此方案相比以往的方案节省了大量纠缠资源,且成功传送的几率达到了1。 相似文献
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通过四个纠缠态粒子来实现未知的三个纠缠态粒子的量子几率隐形传输 总被引:8,自引:2,他引:6
提出一种分别利用四个三态粒子的最大纠缠态和非最大纠缠态作为量子通道来传输一未知的三个三态粒子纠缠态的方案.首先考察量子通道是最大纠缠态的情况,然后进一步考察量子通道是非最大纠缠态的情况,同时发现在后者情况时,通过引进一个辅助粒子,并构造一幺正变换矩阵,即可以一定的几率完成该三态粒子纠缠态的隐形传输. 相似文献
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提出基于三粒子GHZ态的双向量子可控隐形传态方案.方案中,使用两个三粒子GHZ态作为量子通道.而根据在量子通道中发送者,接收者和控制者所拥有的粒子的不同以及所采用的测量基的不同,设计出了三方参与的双向可控量子隐形传态方案和四方参与的双向可控量子隐形传态方案.在方案中,Alice和Bob对所拥有的粒子做合适的投影测量,并将其测量结果通知对方和控制者.若控制者同意此次传态,则会对自己所拥有的粒子做投影测量,并将结果告知接收者.接收者根据发送者和控制者的测量信息,做出相对应的幺正操作来重建发送者的量子态.同时三方参与和四方参与的量子可控隐形传态方案提高了通信的安全性. 相似文献
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提出一种任意两粒子纠缠态1→2普适远程克隆方案. 此方案仅需一个特殊的四粒子纠缠态作为量子信道, 就可使处于空间不同位置的两个接收者分别以5/6的保真度得到任意输入态的近似拷贝, 该保真度远高于已有方案中的保真度. 将方案推广到任意两粒子纠缠态1→N(N>2)普适远程克隆的情况, 可使处于不同地点的N个接收者分别以(2N+1)/(3N)的保真度得到输入态的近似拷贝. 另外, 提出一种以上述单个特殊四粒子纠缠态作为量子信道, 在多目标量子比特受控非门和
关键词:
量子纠缠态
普适远程克隆
保真度 相似文献
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利用两个EPR态完全隐形传输四粒子W态 总被引:2,自引:2,他引:0
为了减少量子隐形传态中的测量次数和运算量,提出了一个利用两个EPR对作为量子信道,实现四粒子W纠缠态的隐形传输的方案.发送者Alice只需利用16个正交完备测量基对要传送的未知四粒子纠缠W态和两个EPR对中属于自己的粒子做一次正交完备基测量,然后将测量所产生的16种塌陷态结果通过经典信道告知接收者,接收者Bob根据这些信息,通过引入两个辅助粒子B3B4,并对手中拥有的粒子做适当的Toffoli门、C-Not门、Pauli-X门、Pauli-Z门变换,就能将16种畸变态全部恢复到发送者Alice欲传送的未知四粒子原始量子态,从而以100%的概率实现四粒子纠缠W态的隐形传输.利用量子力学波函数的叠加原理和变换算符的思想,很容易得出正交完备基测量后的16种塌陷态表达式和接收者Bob所做的由量子门组成的幺正变换的表达式.该方案中由于采用了正交完备基测量的方法,大大减少了发送者所需要做的测量计算,而且整个方案只需要一次正交完备基测量和由各种量子逻辑门组成的简单幺正变换,实现更为容易. 相似文献
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提出了一个利用六粒子最大纠缠态作为纠缠资源的双向量子控制隐形传态方案.该理论方案中,六粒子最大纠缠态作为量子通道来连系着合法的三方——通信双方和控制方,通信双方既是发送方同时也是接收方.传输过程中,Alice传输一个任意单粒子态a给Bob的同时Bob也传输一个任意的单粒子态b给Alice;由控制方Charlie来控制和协助通信双方完成最终的量子态的交换;Bob先对自己手中的粒子作一个幺正操作,用户双方再各自对自己手中的粒子执行Bell基测量,测量完成后通过经典信道将自己的测量结果公开宣布,用户双方根据对方所公布的测量结果做相应的幺正操作,从而成功地实现双向量子控制隐形传态. 相似文献
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提出了一个基于高维2m+1粒子纠缠态的任意m粒子态量子可控离物传态方案,发送方Alice对需传送的未知态量子系统和手中的纠缠粒子执行m个广义Bell基测量,控制方执行广义X基测量,依据预先共享量子纠缠态非定域相关性,接收方对手中的粒子执行相应的幺正操作就可以重建原来未知量子态.与其他方案相比,方案减少了任意高维多粒子态可控离物传送所需传送粒子数.我们进一步讨论了基于纯纠缠信道的概率量子可控离物传态方案,通过与发送方和控制方合作,接收方只需对手中的纠缠粒子和引入的附加粒子执行联合幺正演化和投影测量,就可以在他的粒子上概率的重建原来的未知量子态,最后,方案计算讨论了基于纯纠缠态量子可控离物传态成功概率与信道纠缠度之间的关系. 相似文献
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SHA Jin-Qiao FANG Jian-Xing ZHU Shi-Qun JIANG Wei-Xing QIAN Xue-Min 《理论物理通讯》2006,46(4):595-598
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
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CHENAi-Xi WUShu-Dong 《理论物理通讯》2003,40(6):651-654
In this paper, we propose a protocol where one can realize reestablishment of an unknown state and its orthogonal complement state with a certain probability. In the first stage of the protocol, teleportation is performed between Alice (a sender) and Bob (a receiver) through a nonmaximally entangled quantum channel. In the process of teleportation, Alice performs nonmaximally entangled state measurement. In the second stage of the protocol, Victor(a state preparer) disentangles leftover nonmaximally entangled states by a single-particle measurement. With the assistance of Victor Alice can reestablish the original state or produce its orthogonal state. 相似文献
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A scheme for teleporting an unknown three-particle GHZ state from a sender
to either one of two receivers is proposed. In this scheme, the quantum
channel is composed of two non-maximally three-particle entangled W states. An unknown three-particle GHZ state can be perfectly teleported
probabilistically if the sender performs two generalized Bell-state
measurements and the Hadamard operation while either one of two receivers
introduces an ancillary particle which is one of the final three particle
constituting the teleported state, then performs the controlled-not
operation with the ancillary particle as the target bit and introduces an
appropriate unitary transformation with the help of the other receiver's
simple measurements. All kinds of unitary transformations are given in
detail. The present scheme may be directly generalized to teleport an
unknown multiparticle GHZ state via two three-particle entangled W states
used as the quantum channel. 相似文献
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利用三粒子W态隐形传送三粒子GHZ态 总被引:7,自引:1,他引:6
提出一个三粒子GHZ(Greenberger-Horne-Zeilinger)态从发送者传送给两个接收者中任意一个的量子隐形传送方案。此方案用两个三粒子W态作为量子信道。若发送者进行两次贝尔态测量和阿达码门操作,想得到所需传送的三粒子GHZ态的接收者引进一个辅助粒子,进行控制-非操作,同时根据另一个接收者的测量结果实施一个适当的幺正变换操作,可以一定的概率成功地隐形传送三粒子GHZ态。同时,此方案可推广至隐形传送n粒子GHZ态,这时也只需用两个三粒子W态作为量子信道,但这时想得到所需传送的n粒子GHZ态的接收者需引进(n-2)个辅助粒子,进行(n-2)次控制非操作,同时根据另一个接收者的测量结果实施一个适当的幺正变换操作,可以一定的概率成功地隐形传送n粒子GHZ态。 相似文献
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Probabilistic teleportation of an arbitrary GHZ-class state with a pure entangled two-particle quantum channel and its application in quantum state sharing 总被引:1,自引:0,他引:1 下载免费PDF全文
This paper presents a scheme for probabilistic teleportation of an
arbitrary GHZ-class state with a pure entangled two-particle quantum
channel. The sender Alice first teleports the coefficients of the
unknown state to the receiver Bob, and then Bob reconstructs the
state with an auxiliary particle and some unitary operations if the
teleportation succeeds. This scheme has the advantage of
transmitting much less particles for teleporting an arbitrary
GHZ-class state than
others. Moreover, it discusses the application of this
scheme in quantum state sharing. 相似文献
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In this paper, we propose a protocol where one can realize reestablishment of an unknown state and its orthogonal complement state with a certain probability. In the first stage of the protocol, teleportation is performed between Alice (a sender) and Bob (a receiver) through a nonmaximally entangled quantum channel. In the process of teleportation, Alice performs nonmaximally entangled state measurement. In the second stage of the protocol, Victor (a state preparer) disentangles leftover nonmaximally entangled states by a single-particle measurement. With the assistance of Victor Alice can reestablish the original state or produce its orthogonal state. 相似文献
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Probabilistic Teleportation of an Unknown One-Particle State by a Three-Particle General W State 总被引:3,自引:0,他引:3
XIU Xiao-Ming DONG Li GAO Ya-Jun 《理论物理通讯》2007,47(4):625-628
Two schemes for teleporting an unknown one-particle state are proposed when a general W state is utilized as quantum channel. In the first scheme, after the sender (Alice) makes a Bell-state measurement on her particles, the recipient (Bob) performs a Von Neumann measurement and introduces an auxiliary particle, and carries out a unitary transformation on his particle and the auxiliary particle, and performs a Von Neumann measurement on the auxiliary particle to confirm whether the teleportation succeeds or not. In the second scheme, the recipient (Bob) does not need to perform the first Von Neumann measurement or introduce the auxiliary particle, which is necessary in the first scheme. It is shown that the maxima/probabilities of successful teleportation of the two schemes are identical if the recipient (Bob) performs an appropriate unitary transformation and adopts a proper particle on which he recovers the quantum information of state to be teleported. 相似文献
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Qing Shao 《International Journal of Theoretical Physics》2013,52(8):2573-2577
In this article, a scheme for quantum teleportation of a two-qubit entangled state using four-qubit cluster state is discussed by use of cavity quantum electrodynamics (QED) involving the interaction of the atoms with the cavity. In this protocol, by using a one-dimensional maximally four-qubit cluster state as quantum channel, quantum information of an unknown state of two two-level particles is faithfully transmitted from a sender (Alice) to a remote receiver (Bob). According to the results measured by the Bob, as it is shown, the unknown two-particle entangled state can be teleported perfectly, and the successful possibilities and fidelities of the scheme can reach 1.0. 相似文献
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With an arbitrary bi-particle entangled mixed state which is shared by Alice (the sender) and Bob (the receiver) acted as
a quantum channel, at first, a teleportation protocol that Alice successfully transmits an unknown mixed state to Bob based
on a positive operator-valued measurement (POVM) is presented. The upper bound of probability to teleport successfully an
unknown mixed state is then investigated, and conclude that it completely depends on the entanglement degree of the bi-particle
entangled mixed state as a resource. 相似文献