Nonidentical Coupling-based N-atom W Entanglement

2011-01-15 07:24ZHANGYingqiao
关键词:延吉级联信息学

ZHANG Ying-qiao

(Department of Physics,College of Science,Yanbian University,Yanji 133002,China)

Nonidentical Coupling-based N-atom W Entanglement

ZHANG Ying-qiao

(Department of Physics,College of Science,Yanbian University,Yanji 133002,China)

Based on the nonidentical coupling of N atoms with a single-mode cavity,a scheme for generation of an N-atom W state is proposed in cavity QED.Under the condition of the large-detuned interactionΔ≫gj,the influence of cavity decay is negligible.Such multiple-qubit entanglement will have wide applications to largescale quantum communication and quantum computation.

N-atom W state;three-level atom;cavity QED

1 Introduction

Quantum entanglement is an important physical resource in quantum communication[1-3]and quantum computation.So far,a lot of schemes[4-11]have been proposed to generate entanglements based on various of physical systems both in theory and experiment.Most of these schemes are focused on generation of two-qubit or three-qubit entanglements.For example,Turchette et al[6]have produced the deterministic entangled states of two trapped ions.In this scheme,the two qubits are constituted by the internal states of two trapped ions in both the Bell-like singlet and triplet states.Reina et al[7]have prepared the maximally entangled Bell and Greenberger-Horne-Zeilinger states by optically driven the coupled quantum dots.An alternative scheme[8]to generate three-qubit W state via nonlinear optical state truncation using quantum scissors is proposed.Using atom interferometric techniques,the generation of Bell,NOON and W states of an electromagnetic field in high-Q cavities are also proposed[9].

However,multiple-qubit entanglements are often required to a large-scale quantum information processing.Therefore,the generation of multiple-qubit enanglements have attracted increasingly attentions.For example,an experimental demonstration of five-photon entanglement[10]was provided by generating a four-photon entangled state with two entangled photon pairs and then combining itwith a single-photon state.Based on rf SQUID,a simple scheme was presented to generate the N-qubit W states by adiabatic passage[11].

Based on the nonidentical coupling of the three three-level atoms with a resonant single-mode vacuum cavity field[12]and the large-detuning interaction of two identical two-level atoms with a singlemode cavity field[13]in cavity QED,as well as the combination of the coherent dynamics of the above two schemes[14],we propose a scheme for generation of an N-atom W state.Though it is a generalization of the previous three-atom W state scheme[15],it is universal to multiple-qubit case.

This paper is organized as follows:In Sec.Ⅱ we describe the coupling dynamics of N atoms interaction with a single-mode cavity.In Sec.Ⅲ we describe the generation of an N-atom W state.Conclusion is given in Sec.Ⅳ.

2 Coupling Dynamics of N Atoms Interaction with a Single-mode Cavity

We consider that N three-level atoms simultaneously interact with a single-mode cavity field.Each atom has one excited state|e〉and two ground states|g〉and|r〉.In our scheme,the state|r〉is not involved in the interaction with the cavity mode.In the rotating-wave approximation,the interaction Hamiltonian in the interaction picture can be written as(assumingħ=1)

where S+j=|e〉j〈g|,S-j=|g〉j〈e|(j=1,2,…,N).a†and a are the creation and annihilation operators of the single-mode cavity,respectively.gjis the coupling constant of the j th atom to the cavity mode.Δ=ω0-ωwithω0andωbeing the atomic transition frequency and cavity frequency,respectively.In the case ofΔ≫gj,there is no energy exchange between the atomic system and the cavity,the effective Hamiltonian is

whereλj=g2j/Δandλjk=gjgk/Δ.The first two terms denote the photon-number dependent Stark shifts,and the third term denotes the cavity mode-induced dipole coupling among the N atoms.Assuming that the coupling constant for the first atom with the cavity is g1and the coupling constants for the other atoms with the cavity are g =gj(j=2,3,…,N).If the cavity field is in the vacuum state initially,the effective Hamiltonian becomes

whereλ1=g21/Δand g2/Δ.

3 Generation of an N-atom W State

We assume that the N atoms are in the state〉,initially.The state evolution is

where

If the interaction time satisfy t= (2k+1)π/[(N-1)l+1]λ1(k is an integer)and the parameters that related to nonidentical atom-cavity coupling satisfywe obtain

Therefore we have generated an N-atom W state

4 Conclusion

In conclusion,we have proposed an universal scheme for generation of an N-atom W state based on the nonidentical coupling of N atoms with a single-mode cavity.Under the large-detuned interaction of the N atoms with the single-mode cavity(Δ≫gj),the influence of cavity decay is negligible.Such multiple-qubit entanglements are often required to a large-scale quantum communication and quantum computation.

[1] Bennett C H,Brassard G,Crépeau C,et al.Teleporting an Unknown Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels[J].Phys Rev Lett,1993,70:1895-1899.

[2] Boschi D,Branca S,Martini F D,et al.Experimental Realization of Teleporting an Unknown Pure Quantum State via Dual Classical and Einstein-Podolsky-Rosen Channels[J].Phys Rev Lett,1998,80:1121-1125.

[3] Ekert A K.Quantum Cryptography based on Bell’s Theorem[J].Phys Rev Lett,1991,67:661-663.

[4] Osnaghi S,Bertet P,Auffeves A,et al.Coherent Control of an Atomic Collision in a Cavity[J].Phys Rev Lett,2001,87:037902(4).

[5] Eibl M,Kiesel N,Bourennane M,et al.Experimental Realization of a Three-qubit Entangled W State[J].Phys Rev Lett,2004,92:077901-077904.

[6] Turchette Q A,Wood C S,King B E,et al.Deterministic Entanglement of Two Trapped Ions[J].Phys Rev Lett,1998,81:3631-3634.

[7] Reina J H,Quiroga L,Johnson N F.Quantum Entanglement and Information Processing via Excitons in Optically Driven Quantum Dots[J].Phys Rev A,2000,62:012305(8).

[8] Said R S,Wahiddin M R B,Umarov B A.Generation of Three-qubit Entangled W-state by Nonlinear Optical State Truncation[J].J Phys B:At Mol Opt Phys,2006,39:1269-1274.

[9] Islam R,Khosa A H,Saif F.Generation of Bell,NOON and W states via Atom Interferome-try[J].J Phys B:At Mol Opt Phys,2008,41:035505-035514.

[10] Zhao Z,Chen Y A,Zhang A N,et al.Experimental Demonstration of Five-photon Entanglement and Open-Destination Teleportation[J].Nature,2004,430:54-58.

[11] Deng Z J,Gao K L,Feng M.Generation of N-qubit W States with rf SQUID Qubits by Adiabatic Passage[J].Phys Rev A,2006,74:064303(4).

[12] Shao X Q,Zhu A D,Zhang S,et al.Efficient Scheme for Implementing an N-qubit Toffoli Gate by a Single Resonant Interaction with Cavity Quantum Electrodynamics[J].Phys Rev A,2007,75:034307(4).

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[15] Zhang Y Q.Generation of a Three-qubit W State via Atoms-Cavity Nonidentical Coupling[J].Journal of Yanbian University(Natural Science),2010,36(2):146-148.

1004-4353(2011)03-0242-03

基于非全同耦合的N- 原子W纠缠态

张英俏
(延边大学理学院 物理系,吉林 延吉133002)

在腔QED中利用N个原子与一个单模腔的非全同耦合提出一个制备N原子W纠缠 态的方案.在大失谐相互作用Δ≫gj的条件下,腔衰减的影响可以忽略.此类多比特纠缠态可广泛应用于级联量子通讯和量子计算中.

N原子W态;三能级原子;腔QED

2011 -05 -14

张英俏(1978—),女,理学博士,讲师,研究方向为量子信息学.

0365;4250

A

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