Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage

doi:10.1088/1674-1056/24/7/070310

中国物理B ›› 2015, Vol. 24 ›› Issue (7): 70310-070310.doi: 10.1088/1674-1056/24/7/070310

Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage

张春玲^a, 陈美锋^b

a Department of Electronic and Information Engineering, Sunshine College Fuzhou University, Fuzhou 350002, China;
b Laboratory of Quantum Optics, Department of Physics, Fuzhou University, Fuzhou 350002, China

收稿日期:2014-11-14 修回日期:2014-12-12 出版日期:2015-07-05 发布日期:2015-07-05
基金资助:
Project supported by the Funding (type B) from the Fujian Education Department, China (Grant No. JB13261).

Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage

Zhang Chun-Ling (张春玲)^a, Chen Mei-Feng (陈美锋)^b

a Department of Electronic and Information Engineering, Sunshine College Fuzhou University, Fuzhou 350002, China;
b Laboratory of Quantum Optics, Department of Physics, Fuzhou University, Fuzhou 350002, China

Received:2014-11-14 Revised:2014-12-12 Online:2015-07-05 Published:2015-07-05
Contact: Zhang Chun-Ling E-mail:mzhangchunling@163.com
Supported by:
Project supported by the Funding (type B) from the Fujian Education Department, China (Grant No. JB13261).

摘要/Abstract

摘要： We propose a new approach for quantum state transfer (QST) between atomic ensembles separately trapped in two distant cavities connected by an optical fiber via adiabatic passage. The three-level Λ-type atoms in each ensemble dispersively interact with the nonresonant classical field and cavity mode. By choosing appropriate parameters of the system, the effective Hamiltonian describes two atomic ensembles interacting with “the same cavity mode” and has a dark state. Consequently, the QST between atomic ensembles can be implemented via adiabatic passage. Numerical calculations show that the scheme is robust against moderate fluctuations of the experimental parameters. In addition, the effect of decoherence can be suppressed effectively. The idea provides a scalable way to an atomic-ensemble-based quantum network, which may be reachable with currently available technology.

关键词: quantum state transfer, atomic ensemble, cavity QED

Abstract: We propose a new approach for quantum state transfer (QST) between atomic ensembles separately trapped in two distant cavities connected by an optical fiber via adiabatic passage. The three-level Λ-type atoms in each ensemble dispersively interact with the nonresonant classical field and cavity mode. By choosing appropriate parameters of the system, the effective Hamiltonian describes two atomic ensembles interacting with “the same cavity mode” and has a dark state. Consequently, the QST between atomic ensembles can be implemented via adiabatic passage. Numerical calculations show that the scheme is robust against moderate fluctuations of the experimental parameters. In addition, the effect of decoherence can be suppressed effectively. The idea provides a scalable way to an atomic-ensemble-based quantum network, which may be reachable with currently available technology.

Key words: quantum state transfer, atomic ensemble, cavity QED

中图分类号: (Entanglement production and manipulation)

03.67.Bg

42.50.Dv (Quantum state engineering and measurements) 42.50.Pq (Cavity quantum electrodynamics; micromasers)

张春玲, 陈美锋. Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage[J]. 中国物理B, 2015, 24(7): 70310-070310.

Zhang Chun-Ling (张春玲), Chen Mei-Feng (陈美锋). Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage[J]. Chin. Phys. B, 2015, 24(7): 70310-070310.

参考文献 41

[1]	Lloyd S 1993 Science 261 1569
[2]	Bennett C H, Brassard G, Crépeau C, Jozsa R, Peres A and Wootters W K 1993 Phys. Rev. Lett. 70 1895
[3]	Gisin N, Ribordy G, Tittel W and Zbinden H 2002 Rev. Mod. Phys. 74 145
[4]	Ekert A K 1991 Phys. Rev. Lett. 67 661
[5]	Karlsson A and Bourennane M 1998 Phys. Rev. A 58 4394
[6]	Brune M, Hagley E, Dreyer J, Maitre X, Maali A, Wunderlich C, Raimond J M and Haroche S 1996 Phys. Rev. Lett. 77 4887
[7]	Turchette Q A, Hood C J, Lange W, Mabuchi H and Kimble H J 1995 Phys. Rev. Lett. 75 4710
[8]	Mattle K, Weinfurter H, Kwiat P G and Zeilinger A 1996 Phys. Rev. Lett. 76 4656
[9]	Bennett C H and Wiesner S J 1992 Phys. Rev. Lett. 69 2881
[10]	Cirac J I, Zoller P, Kimble H J and Mabuchi H 1997 Phys. Rev. Lett. 78 3221
[11]	Christandl M, Datta N, Ekert A and Landahl A J 2004 Phys. Rev. Lett. 92 187902
[12]	Yao N Y, Jiang L, Gorshkov A V, Gong Z X, Zhai A, Duan L M and Lukin M D 2011 Phys. Rev. Lett. 106 040505
[13]	Shi Z C, Xia Y, Song J and Song H S 2011 J. Opt. Soc. Am. B 28 2909
[14]	Vitanov N V, Halfmann T, Shore B W and Bergmann K 2001 Annu. Rev. Phys. Chem. 52 763
[15]	Bergmann K, Theuer H and Shore B W 1998 Rev. Mod. Phys. 70 1003
[16]	Vitanov N V, Suominen K A and Shore B W 1999 J. Phys. B 32 4535
[17]	Lacour X, Sangouard N, Guérin S and Jauslin H R 2006 Phys. Rev. A 73 042321
[18]	Talab M A, Guérin S and Jauslin H R 2005 Phys. Rev. A 72 012339
[19]	Talab M A, Guérin S, Sangouard N and Jauslin H R 2005 Phys. Rev. A 71 023805
[20]	Zheng A S, Liu L B and Chen H Y 2011 Chin. Phys. Lett. 28 080303
[21]	Yang Z B, Wu H Z and Zheng S B 2010 Chin. Phys. B 19 094205
[22]	Song J, Xia Y and Song H S 2010 Appl. Rev. Lett. 96 071102
[23]	Serafini A, Mancini S and Bose S 2006 Phys. Rev. Lett. 96 010503
[24]	Hammerer K, Sorensen A S and Polzik E S 2010 Rev. Mod. Phys. 82 1041
[25]	Holstein T and Primakoff H 1940 Phys. Rev. 58 1098
[26]	Kuklinski J R, Gaubatz U, Hioe F T and Bergmann K 1989 Phys. Rev. A 40 6741
[27]	Shen L T, Wu H Z and Yang Z B 2012 Eur. Phys. J. D 66 123
[28]	Zhang C L, Li W Z and Chen M F 2013 Opt. Commun. 311 301
[29]	Lu M, Xia Y, Song J and An Z B 2013 J. Opt. Soc. Am. B 30 2142
[30]	Boozer A D, Boca A, Miller R, Northup T E and Kimble H J 2006 Phys. Rev. Lett. 97 083602
[31]	Boca A, Miller R, Birnbaum K M, Boozer A D, McKeever J and Kimble H J 2004 Phys. Rev. Lett. 93 233603
[32]	McKeever J, Buck J R, Boozer A D, Kuzmich A, Nagerl H C, Stamper-Kurn D M and Kimble H J 2003 Phys. Rev. Lett. 90 133602
[33]	Yin Z Q and Li F L 2007 Phys. Rev. A 75 012324
[34]	Spillane S M, Kippenberg T J, Painter O J and Vahala K J 2003 Phys. Rev. Lett. 91 043902
[35]	Yuan L B and Zhou L M 1998 Appl. Opt. 37 4168
[36]	Dragone C, Henry C H, Kaminow I P and Kistler R C 1989 IEEE Photon. Technol. Lett. 1 241
[37]	Duan L M, Lukin M, Cirac I and Zoller P 2001 Nature 414 413
[38]	Reiter F and Sorensen A S 2012 Phys. Rev. A 85 032111
[39]	Zheng S B 2012 Phys. Rev. A 86 013828
[40]	Spillane S M, Kippenberg T J, Vahala K J, Goh K W, Wilcut E and Kimble H J 2005 Phys. Rev. A 71 013817
[41]	Hartmann M J, Brandao F G S L and Plenio M B 2006 Nat. Phys. 2 849

Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage

Quantum state transfer between atomic ensembles trapped in separate cavities via adiabatic passage

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