吉林大学学报(理学版)

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利用原子和光腔作用实现受控非门

杨红1, 吴伟1, 符运良1, 彭鸿雁1, 张廷桂2   

  1. 1. 海南师范大学 物理与电子工程学院, 海口 571158; 2. 海南师范大学 数学与统计学院, 海口 571158
  • 收稿日期:2014-04-04 出版日期:2015-01-26 发布日期:2015-01-19
  • 通讯作者: 张廷桂 E-mail:tinggui333@163.com

Implementation of CNOT Gate in an Optical Cavity with Atoms

YANG Hong1, WU Wei1, FU Yunliang1, PENG Hongyan1, ZHANG Tinggui2   

  1. 1. College of Physics and Electronic Engineering, Hainan Normal University, Haikou 571158, China;2. School of Mathematics and Statistics, Hainan Normal University, Haikou 571158, China
  • Received:2014-04-04 Online:2015-01-26 Published:2015-01-19
  • Contact: ZHANG Tinggui E-mail:tinggui333@163.com

摘要:

分别在2个基态|g1〉和|g2〉上制备2个相同的五能级Λ型原子, 再将其通过一个双模(a模和b模)光腔, 其中a模光子耦合下能级|g〉到中间能级|e〉的跃迁, b模光
子耦合中间能级|e〉到上能级|f〉的跃迁, 耦合强度分别为ga和gb. 将信息编码在腔模的偏振光子态上, 在原子通过光腔后测量腔的偏振光子态. 数值计算结果表明: 通过控制原子与内腔场的相互作用时间可实现受控非门; 当单光子失谐Δ=0.5g, g/k=2~10时, 保真度均大于99%.

关键词: 量子计算机, 受控非门, 腔量子电动力学, 保真度, 光子

Abstract:

First, we prepared two fivelevel Λtype atoms in ground states |g1〉and |g1〉.Next we let them pass through this doublemode (a mode and b mode) optical cavity. And amode couples with the transition |g〉→|e〉, bmode couples with the transition |e〉→|f〉, with the coupling strength ga and gb respectively. We coded the information on the polarized photon states to measure the cavity polarization states after the atoms passed through the cavity. The C-NOT gate is realized by controlling the interaction time of atoms and intracavity fields. High fidelity and low photon loss can be realized by selecting reasonable parameters. The numerical results show that to realize CNOT gate, the cavity with a strong coupling and little decay is necessary. When we set singlephoton detuning Δ=0.5g, and g/k is from 2 to 10, the fidelity can be keeping over 99%.

Key words: quantum computer, CNOT gate, cavity QED, fidelity, photon loss

中图分类号: 

  • O431.2