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本文在级联四波混频结构基础上, 利用光学分束器作为反馈控制器理论构造了一种相干反馈控制系统. 考虑相干反馈回路中光束传输损耗以及原子对光束吸收损耗, 通过计算系统的协方差矩阵以及利用部分转置正定判据, 分析了该系统在不同反馈强度、增益以及相位下的纠缠特性. 结果表明, 系统存在真正的三组份纠缠, 但是反馈控制器过度反馈会破坏系统的三组份量子纠缠特性. 另外, 将相位设为180°, 通过适当改变增益大小以及在0.1—0.4范围内调节分束器反射率的大小可以增强系统的量子纠缠程度. 本文为实验上基于级联四波混频相干反馈控制系统制备多组份纠缠奠定理论基础, 在量子通信领域有着潜在应用.Based on the cascaded four wave mixing processes, a coherent-feedback control system is constructed by utilizing a linear beam splitter as the feedback controller. Considering the loss of optical propagation in the coherent feedback loop and the absorption effect of Rb vapor cells to beams, we theoretically investigate the entanglement properties of this system under different feedback ratio, gain and phase by calculating the covariance matrix of system and applying the positivity under partial transpose (PPT) criterion to all possible bipartitions. The result shows that the genuine tripartite entanglement exists in the coherent feedback control system, but the entanglement structure of system will be destroyed by the excessive feedback. In addition, when the phase is π, we find that the tripartite entanglement can be enhanced by changing the gains and the reflectivity of the beam splitter in the range of 0.1 to 0.4. The results pave the way for manipulating multipartite entanglement by coherent feedback control and have potential application in quantum communication.
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Keywords:
- four wave mixing /
- coherent feedback /
- quantum entanglement
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[33] Wiseman H M, Jones S J, Doherty A C 2007 Phys. Rev. Lett. 98 140402Google Scholar
[34] Jasperse M 2010 M. S. Thesis (Melbourne: The University of Melbourne)
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图 1 (a)级联四波混频相干反馈控制系统简图; (b)85Rb原子D1线的双Λ型跃迁能级结构图能级图. ∆对应单光子失谐, δ对应双光子失谐
Fig. 1. (a) The scheme of coherent feedback control system based on the cascade four wave mixing processes; (b) The Double-Λ type transition energy-level diagram of 85Rb D1 line. ∆ corresponds to one-photon detuning, δ corresponds to two-photon detuning.
图 4 (a)(b)(c)(d)分别为四种铷池增益情形下系统的三个输出光场强度随相位ϕ的变化. 这里, k = 0.5,
$ {\hat N_1} = \hat a_3^{'\dagger }\hat a_3^{'}$ ,${\hat N_2} = \hat b_2^{'\dagger }\hat b_2^{'} $ ,${\hat N_3} = \hat c_1^{\dagger} {\hat c_1} $ Fig. 4. (a)(b)(c)(d) show the relationship between the intensity of three output fields and the phase ϕ under different gains condition, respectively. Here, k = 0.5,
$ {\hat N_1} = \hat a_3^{'\dagger }\hat a_3^{'}, \;{\hat N_2} = \hat b_2^{'\dagger }\hat b_2^{'}, \;{\hat N_3} = \hat c_1^{\dagger} {\hat c_1}$ . -
[1] DiVincenzo D P 1995 Science 270 255Google Scholar
[2] Lloyd S, Braunstein S L 1999 Phys. Rev. Lett. 82 1784Google Scholar
[3] Braunstein S L, Loock P van 2005 Rev. Mod. Phys. 77 513Google Scholar
[4] Weedbrook C, Pirandola S, García-Patrón R, Cerf N J, Ralph T C, Shapiro J H, Lloyd S 2012 Rev. Mod. Phys. 84 621Google Scholar
[5] Bennett C H, Wiesner S J 1992 Phys. Rev. Lett. 69 2881Google Scholar
[6] Jing J, Zhang J, Yan Y, Zhao F, Xie C, Peng K 2003 Phys. Rev. Lett. 90 167903Google Scholar
[7] Yonezawa H, Braunstein S L, Furusawa A 2007 Phys. Rev. Lett. 99 110503Google Scholar
[8] Jia X, Su X, Pan Q, Gao J, Xie C, Peng K 2004 Phys. Rev. Lett. 93 250503Google Scholar
[9] Yonezawa H, Aoki T, Furasawa A 2004 Nature 431 430Google Scholar
[10] Loock P van, Braunstein S L 2000 Phys. Rev. Lett. 84 3482Google Scholar
[11] Coelho A S, Barbosa F A S, Cassemiro K N, Villar A S, Martinelli M, Nussenzveig P 2009 Science 326 823Google Scholar
[12] Armstrong S, Wang M, Teh R Y, Gong Q, He Q, Janousek J, Bachor H A, Reid M D, Lam P K 2015 Nat. Phys. 11 167Google Scholar
[13] Cassemiro K N, Villar A S 2008 Phys. Rev. A 77 022311Google Scholar
[14] Daems D, Cerf N J 2010 Phys. Rev. A 82 032303Google Scholar
[15] Yokoyama S, Ukai R, Armstrong S C, et al. 2013 Nat. Photonics 7 982Google Scholar
[16] Roslund J, de Araújo R M, Jiang S, Fabre C, Treps N 2014 Nat. Photonics 8 109Google Scholar
[17] McCormick C F, Boyer V, Arimondo E, Lett P D 2007 Opt. Lett. 32 178Google Scholar
[18] Wang W, Cao L, Lou Y, Du J, Jing J 2018 Appl. Phys. Lett. 112 034101Google Scholar
[19] Lv S, Jing J 2018 Opt. Commun. 424 63Google Scholar
[20] Lv S, Jing J 2017 Phys. Rev. A 96 043873Google Scholar
[21] Wang H, Zheng Z, Wang Y, Jing J 2016 Opt. Express 24 23459Google Scholar
[22] Zhang K, Wang W, Liu S, Pan X, Du J, Lou Y, Yu S, Lv S, Treps N, Fabre C, Jing J 2020 Phys. Rev. Lett. 124 090501Google Scholar
[23] Zhou Y, Jia X, Li F, Xie C, Peng K, 2015 Opt. Express 23 4952Google Scholar
[24] Bechhoefer J 2005 Rev. Mod. Phys. 77 783Google Scholar
[25] Wiseman H M, Milburn G J 1994 Phys. Rev. A 49 4110Google Scholar
[26] Nelson R J, Weinstein Y, Cory D, Lloyd S 2000 Phys. Rev. Lett. 85 3045Google Scholar
[27] Lloyd S 2000 Phys. Rev. A 62 022108Google Scholar
[28] Kerckhoff J, Nurdin H I, Pavlichin D S, Mabuchi H 2010 Phys. Rev. Lett. 105 040502Google Scholar
[29] Iida S, Yukawa M, Yonezawa H, Yamamoto N, Furasawa A 2012 IEEE Trans. Autom. Control 57 2045Google Scholar
[30] Pan X, Chen H, Wei T, Zhang J, Marino A M, Treps N, Glasser R T, Jing J 2018 Phys. Rev. B 97 161115Google Scholar
[31] Jasperse M, Turner L D, Scholten R E 2011 Opt. Express 19 3765Google Scholar
[32] Fox M 2006 Quantum Optics: An Introduction (New York: Oxford University Press)
[33] Wiseman H M, Jones S J, Doherty A C 2007 Phys. Rev. Lett. 98 140402Google Scholar
[34] Jasperse M 2010 M. S. Thesis (Melbourne: The University of Melbourne)
[35] Simon R 2000 Phys. Rev. Lett. 84 2726Google Scholar
[36] Duan L M, Giedke G, Cirac J I, Zoller P 2000 Phys. Rev. Lett. 84 2722Google Scholar
[37] Werner R F, Wolf M M 2001 Phys. Rev. Lett. 86 3658Google Scholar
[38] Barbosa F A S, Coelho A S, Muñoz-Martínez L F, et al. 2018 Phys. Rev. Lett. 121 073601Google Scholar
[39] Qin Z, Cao L, Wang H, Marino A M, Zhang W, Jing J 2014 Phys. Rev. Lett. 113 023602Google Scholar
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