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1.
We propose an experimentally feasible teleportation scheme with three-atom W-class state, which was first proposed by Agrawal and Pati [P. Agrawal and A. Pati, Phys. Rev. A 74 (2006) 062320 ], in cavity QED. In this scheme atoms interact simultaneously with a nonresonant cavity and there is no energy exchange between the atoms and the cavity. Thus it is insensitive to the cavity decay, which is of importance in view of experiment.  相似文献   

2.
    
A scheme for approximately and conditionally teleporting an unknown atomic state in dissipative cavity QED is proposed. It is the extension of the scheme of [Phys. Rev. A 69 (2004) 064302], where the cavity mode decay has not been considered and only a time point of system evolution and the corresponding fidelity implementing the teleportation are given. In fact, the cavity mode decay exists really and must be delt with. In this paper, we investigate the influence from the cavity mode decay on the implementation of the approximate and conditional teleportation by means of the dissipative Jaynes Cummings model and then show the analytical expression of the fidelity of realization of the teleportation. Alternatively, our scheme does not involve an additional atom, only requiring two atoms and one single-mode cavity.  相似文献   

3.
In this paper, we present a peculiar tripartite entangled state that is inequivalent to both the GHZ state and the W state, and then propose to implement efficient quantum information processing such as quantum dense coding and teleportation with this entangled state in cavity QED. In this scheme the atoms interact with a highly detuned cavity field with the assistance of a strong classical driven field. It does not require the transfer of quantum information between the atomic system and the cavity, and then our scheme is insensitive to both the cavity decay and the thermal field.  相似文献   

4.
We propose a scheme for approximately and conditionally teleporting an unknown atomic-entangled state in dissipative cavity QED. It is the further development of the scheme of [Phys. Rev. A 69 (2004) 064302], where the cavity mode decay has not been considered and the state teleportated is an unknown atomic state. In this paper, we investigate the influence of the decay on the approximate and conditional teleportation of the unknown atomic-entangled state, which is different from that teleportated in [Phys. Rev. A 69 (2004) 064302] and then give the fidelity of the teleportation, which depends on the cavity mode decay. The scheme may be generalized to not only the teleportation of the cavity-mode-entangled-state by means of a single atom but also the teleportation of the unknown trapped-ionentangled-state in a linear ion trap.  相似文献   

5.
    
In this paper, a scheme is proposed for realization of two-qubit controlled-not gates and teleportation of an entangled state of atom-cavity. In this scheme, applying hyperfine levels of atom, we consider A-type three-level atom interacting resonantly or nonresonantly with cavity field that is prepared in σ- polarized. We consider the experimental feasibility of this scheme and compare our results with other schemes.  相似文献   

6.
    
A scheme is proposed for the controlled teleportation of an arbitrary two-atom state via special W-type entangled states and QED cavity. The scheme does not involve the direct joint Bell-state-measurement (BSM). We show that the quantum information is split into two parts~ thus the original atomic state cannot be perfectly restored by the receiver without the other agent's collaboration and classical communication. In addition, the physical realization of this scheme is not difficult.  相似文献   

7.
    
We put forward an experimentally feasible protocol for realizing a perfect teleportation by using a class of W-state in QED. The simple way of generating the entangled channel and distinguishing the measurement bases is the distinct feature of our scheme. In addition, the probability of teleportation is up to 100%. The scheme can be implemented by the present cavity QED techniques.  相似文献   

8.
提出了一种外场驱动下在腔QED中实现任意两原子态隐形传送的方案.在隐形传送的过程中.以两原子最大纠缠态作为量子通道,不用考虑腔场耗散和外界热场环境的影响.在传送过程中包含着对原子的Bell基测量,但不需要直接进行Bell基测量,而且最终能成功实现传送的几率为1.0.同时这种方案也可以用来传送未知的三原子GHZ态,传送的几率也为1.0.  相似文献   

9.
    
We propose an experimentally feasibleteleportation scheme with three-atom W-class state, which was firstproposed by Agrawal and Pati [P. Agrawal and A. Pati, Phys. Rev. A74 (2006) 062320], in cavity QED. In this scheme atoms interactsimultaneously with a nonresonant cavity and there is no energyexchange between the atoms and the cavity. Thus it is insensitive tothe cavity decay, which is of importance in view of experiment.  相似文献   

10.
    
We propose a scheme for approximately and conditionally teleporting an unknown atomic-entangled state in dissipative cavity QED. Itis the further development of the scheme of [Phys. Rev. A 69 (2004) 064302], where the cavity mode decay has not been considered and thestate teleportated is an unknown atomic state. In this paper, we investigatethe influence of the decay on the approximate and conditional teleportation of the unknown atomic-entangled state, which is different from that teleportatedin [Phys. Rev. A 69 (2004) 064302] and then give the fidelity ofthe teleportation, which depends on the cavity mode decay. The schememay be generalized to not only the teleportation of thecavity-mode-entangled-state by means of a single atom but also theteleportation of the unknown trapped-ion-entangled-state in a linear ion trap.  相似文献   

11.
Teleportation schemes with a tripartite entangled state in cavity QED are investigated. The schemes do not need Bell state measurements and the successful probabilities reach optimality. In addition, the schemes are insensitive to both the cavity decay and the thermal field. We first consider two teleportation schemes via a tripartite GHZ state.The first one is a controlled one for an unknown single-qubit state. The second scheme is teleportation of unknown two-atom entangled state. Then we consider teleporting of single-qubit arbitrary state via a tripartite W state.  相似文献   

12.
本文提出了一个基于腔QED的隐形传送四比特团簇类态方案,在该方案中选用两个GHZ纠缠对作为量子通道,通过对原子和腔场的大失谐作用以及外加强经典场的辅助,可以制备纠缠的量子通道,完成联合的三粒子测量,成功地实现隐形传送四比特团簇类态。结果还表明,此方案不受腔场退相干和热场的影响.  相似文献   

13.
  总被引:4,自引:0,他引:4       下载免费PDF全文
杨贞标 《中国物理》2007,16(2):329-334
An alternative scheme is presented for teleportation of a two-atomentangled state in cavity quantum electrodynamics (QED). It is basedon the resonant atom--cavity field interaction. In the scheme, onlyone cavity is involved, and the number of the atoms needed to bedetected is decreased compared with the previous scheme. Since theresonant atom--cavity field interaction greatly reduces theinteraction time, the decoherence effect can be effectivelysuppressed during the teleportation process. The experimentalfeasibility of the scheme is discussed. The scheme can easily begeneralized to the teleportation of N-atomGreeninger--Horne--Zeilinger (GHZ) entangled states. The number ofatoms needed to be detected does not increase as the number of theatoms in the GHZ state increases.  相似文献   

14.
    
In this paper, we present a peculiartripartite entangled state that isinequivalent to both the GHZ state and the W state, and then propose toimplement efficient quantum information processing such as quantum densecoding and teleportation with this entangled state in cavity QED. In thisscheme the atoms interact with a highly detuned cavity field with theassistance of a strong classical driven field. It does not require thetransfer of quantum information between the atomic system and the cavity,and then our scheme is insensitive to both the cavity decay and the thermal field.  相似文献   

15.
A probabilistic teleportation scheme for atomic state via cavity QED [Phys. Rev. A 70 (2004) 054303] is revisited and accordingly some improvements are made.  相似文献   

16.
We have proposed an alternative scheme for teleportation of two-atom entangled state in cavity QED. It is based on the degenerate Raman interaction of a single-mode cavity field with a ∧-type three-level atom. The prominent feature of the scheme is that only one cavity is required, which is prior to the previous one. Moreover, the atoms need to be detected are reduced compared with the previous scheme. The experimental feasibility of the scheme is discussed.The scheme can easily be generalized for teleportation of N-atom GHZ entangled states. The number of the atoms needed to be detected does not increase as the number of the atoms in GHZ state increases.  相似文献   

17.
    
Teleportation schemes with a tripartite entangled state in cavity QED are investigated. The schemes do not need Bell state measurements and the successful probabilities reach optimality. In addition, the schemes are insensitive to both the cavity decay and the thermal field. We first consider two teleportation schemes via a tripartite GHZ state. The first one is a controlled one for an unknown single-qubit state. The second scheme is teleportation of unknown two-atom entangled state. Then we consider teleporting of single-qubit arbitrary state via a tripartite W state.  相似文献   

18.
    
We have proposed an alternative scheme for teleportation of two-atom entangled state in cavity QED. It is based on the degenerate Raman interaction of a single-mode cavity field with a A-type three-level atom. The prominent feature of the scheme is that only one cavity is required, which is prior to the previous one. Moreover, the atoms need to be detected are reduced compared with the previous scheme. The experimental feasibility of the scheme is discussed. The scheme can easily be generalized for teleportation of N-atom GHZ entangled states. The number of the atoms needed to be detected does not increase as the number of the atoms in GHZ state increases.  相似文献   

19.
  总被引:1,自引:0,他引:1  
A probabilistic teleportation scheme for atomic stats via cavity QED [Phys. Rev. A 70 (2004) 054303] is revisited and accordingly some improvements are made.  相似文献   

20.
We propose a scheme for teleporting a single qubit state employing a unique three-particle W state as quantum channel. By adopting QED cavity technologies, our scheme does not involve the Bell-state measurements(BMs). An unknown state a|0〉 + b|1〉 can be probabilistically teleported by communicators' single particle measurements, unitary operations and classical communications. We can perfectly teleport quantum state ½1√2(|0〉 +|1〉) with 100% probability.  相似文献   

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