欢迎登录材料期刊网

材料期刊网

高级检索

提出了一个利用处在线性阱中的两个全同的三能级离子与两个不同频率的激光脉冲共振相互作用来实现两比特量子SWAP门的方案,该方案是根据Haffner和Riebe等的实验方法与结果选择40Ca+离子S1/2基态的一个塞曼能级作为基态,以亚稳态D5/2的两个塞曼能级作为两个激发态来实现的,选择适当的参数如质心模的频率v=1.2 MHz,拉比频率Ω=0.1v以及Lamb-Dicke参数η=0.1,计算出实现该方案所用的总时间为T≈1.3×10-3S,该时间远小于亚稳态D5/2的寿命T1≈1.16 S,并且在这个方案里消相干是可以被忽略的.在目前的离子阱技术条件下,该方案是可以实现的.

A novel scheme for realizing a two-qubit quantum SWAP gate in ion-trap systems is proposed. Two three-level ions are considered which are confined in a linear trap interacting with two different frequency laser pulse in the case of resonance. According to the experimental methods and results of Haffner and Riebe, one Zeeman level of the S1/2 ground state of 40Ca+ ion can act as one ground state, while two Zeeman levels of the metastable D5/2 state as the excited states.With choosing appropriate parameters such as V=1.2 MHz, Ω=0.1 V and η=0.1, the total timerequired to complete the procedure is T ≈1.3~10-3s, much shorter than the lifetime Tl≈1.16 sof the metastable D5/2 state, and in this scheme decoherence is negligible. Thus this scheme may be realized with presently available ion-trap techniques.

参考文献

[1] Sleator T,Weinfurter H.Realizable universal quantum logic gates[J].Phys.Rev.Lett.,1995,74:4087-4090.
[2] Su Xiaoqin,Guo Guangcan.Quantum communication and quantum computation[J].Chinese Journal of Quantum Electronics (量子电子学报),2004,21(6):706-716 (in Chinese).
[3] Wang X C,Wang C C,Fang S D.On nonlocal quantum gates[J].Chinese Journal of Quantum Electronics (量子电子学报),2005,22(3):392-395 (in Chinese).
[4] Zheng Shibiao,Guo Guangcan.Eifficient scheme for two-atom entanglement and quantum information processing in cavity QED[J].Phys.Rev.Lett.,2000,85:2392-2395.
[5] Khaneja N,et al.Time optimal control in spins systems[J].Phys.Rev.A,2001,63:032308-1-13.
[6] Wang Shunjin,et al.Physical realization of quantum C-NOT gate[J].Chin.Phys.Lett.,2008,25(3):813-816.
[7] Cirac J I,Zoller P.Quantum computations with cold trapped ions[J].Phys.Rev.Lett.,1995,74:4091-4094.
[8] Yang C P,Chu S I.Quantum state transfer and logic gates with two 3-level atoms in cavity QED[J].Phys.A,2004,339:347-353.
[9] Fujiwara Shingo,Hasegawa Shuichi.General method for realizing the conditional phase-shift gate and a simulation of Grover's algorithm in an ion-trap system[J].Phys.Rev.A,2005,71:012337-1-6.
[10] Zheng Shibiao.High-speed geometric quantum phase gates for trapped ions in thermal motion[J].Phys.Rev.A,2006,74:032322-1-4.
[11] Liang L M,Li C Z.Realization of quantum SWAP gate between flying and stationary qubits[J].Phys.Rev.A,2005,72:024303-1-4.
[12] Yang Chuiping,Chu S I.Possible realization of entanglement,logical gates,and quantum-information transfer with superconducting-quantum-interference-device qubits in cavity QED[J].Phys.Rev.A,2003,67,042311-1-4.
[13] Yavuz D D.Single photon SWAP gate using electromagnetically induced transparency[J].Phys.Rev.A,2005,71:053816-1-4.
[14] Yin Zhangqi,Li Fuli.Multiatom and resonant interaction scheme for quantum state transfer and logical gates between two remote cavities via an optical fiber[J].Phys.Rev.A,2007,75:012324-1-11.
[15] Cernoch Antonm,Soubusta Jan,et al.Experimental realization of linear-optical partial SWAP gates[J].Phys.Rev.Lett.,2008,100:180501-1-4.
[16] Lazarou C,Garraway B M.Adiabatic entanglement in two-atom cavity QED[J].Phys.Rev.A,2008,77:023818-1-9.
[17] Chen Tumiao,Nie Zongxiu.Characteristics of trapped ion considering the double frequency of trap field in Paul trap[J].Chinese Journal of Quantum Electronics (量子电子学报),2003,20(1):51-54 (in Chinese).
[18] Haffner H,et al.Scalable multiparticle entanglement of the trapped ions[J].Nature,2005,438:643-646.
[19] Riebe M,et al.Deterministic quantum teleportation with atoms[J].Nature,2004,429:734-737.
[20] Reichle R,et al.Experimental purification of two-atom entanglement[J].Nature,2006,443:838-841.
上一张 下一张
上一张 下一张
计量
  • 下载量()
  • 访问量()
文章评分
  • 您的评分:
  • 1
    0%
  • 2
    0%
  • 3
    0%
  • 4
    0%
  • 5
    0%