Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction

doi:10.1088/1674-1056/19/4/044203

中国物理B ›› 2010, Vol. 19 ›› Issue (4): 44203-044203.doi: 10.1088/1674-1056/19/4/044203

Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction

郑仕标

Department of Physics and State Key Laboratory Breeding Base of Photocatalysis, Fuzhou University, Fuzhou 350002, China

收稿日期:2009-06-24 修回日期:2009-07-05 出版日期:2010-04-15 发布日期:2010-04-15
基金资助:
Project supported by the National Natural Science Foundation of China (Grant No. 10674025) and the Doctoral Foundation of the Ministry of Education of China (Grant No.~20070386002).

Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction

Zheng Shi-Biao(郑仕标)^†

Department of Physics and State Key Laboratory Breeding Base of Photocatalysis, Fuzhou University, Fuzhou 350002, China

Received:2009-06-24 Revised:2009-07-05 Online:2010-04-15 Published:2010-04-15
Supported by:
Project supported by the National Natural Science Foundation of China (Grant No. 10674025) and the Doctoral Foundation of the Ministry of Education of China (Grant No.~20070386002).

摘要/Abstract

摘要： This paper proposes a scheme for generating arbitrary superpositions of several coherent states along a straight line for a cavity mode. In the scheme, several atoms are sent through a cavity initially in a strong coherent state. The superposition of several coherent states with desired coefficients may be generated if each atom is detected in the excited state after it exits the cavity. The scheme is based on resonant atom--cavity interaction and no classical field is required during and after the atom--cavity interaction. Thus, the scheme is very simple and the interaction time is very short, which is important in view of decoherence.

Abstract: This paper proposes a scheme for generating arbitrary superpositions of several coherent states along a straight line for a cavity mode. In the scheme, several atoms are sent through a cavity initially in a strong coherent state. The superposition of several coherent states with desired coefficients may be generated if each atom is detected in the excited state after it exits the cavity. The scheme is based on resonant atom--cavity interaction and no classical field is required during and after the atom--cavity interaction. Thus, the scheme is very simple and the interaction time is very short, which is important in view of decoherence.

Key words: superposition of coherent states, cavity mode, resonant interaction

中图分类号: (Cavity quantum electrodynamics; micromasers)

42.50.Pq

32.80.-t (Photoionization and excitation)

郑仕标. Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction[J]. 中国物理B, 2010, 19(4): 44203-044203.

Zheng Shi-Biao(郑仕标). Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction[J]. Chin. Phys. B, 2010, 19(4): 44203-044203.

参考文献 17

[1]	Vogel K, Akulin V M and Schleich W P 1993 Phys. Rev. Lett. 71 1816
[2]	Parkins A S, Marte P, Zoller P and Kimble H J 1993 Phys. Rev. Lett. 71 3095
[3]	Law C K and Eberly J H 1996 Phys. Rev. Lett.76 1055
[4]	Yurke B and Stoler D 1986 Phys. Rev. Lett.57 13
[5]	Yia Y and Guo G 1989 Phys. Lett. A 136 281
[6]	Janszky J, Domokos P and Aam P 1995 Phys. Rev. A 51 4191
[7]	Szabo S, Adam P, Janszky J and Domokos P 1996 Phys. Rev. A 53 2698
[8]	Brune M, Haroche S, Raimond J M, Davidovich L and Zagury N 1992 Phys. Rev. A 45 5193
[9]	Garraway B M, Sherman B, Moya-Cessa H, Knight P L and Kurizki G 1994 Phys. Rev. A 49 535
[10]	Guo G C and Zheng S B 1996 Phys. Lett. A 223 332
[11]	Lutterbach L G and Davidovich L 2000 Phys. Rev. A 61] 023813
[12]	Zhou L, Song H S, Li C and Guo Y Q 2003 Chin. Phys. 12 45
[13]	Solano E, Agarwal G S and Walther H 2003 Phys. Rev. Lett. 90 027903
[14]	Zheng S B 2007 Phys. Rev. A 75 032114
[15]	Janszky J and Vinogradov A V 1990 Phys. Rev. Lett. 64 2771
[16]	Meunier T, Gleyzes S, Maioli P, Auffeves A, Nogues G, Brune M, Raimond J M and Haroche S 2005 Phys. Rev. Lett.94 010401
[17]	Kuhr S, Gleyzes S, Guerlin C, Bernu J, Hoff U B, Deleglise S, Osnaghi S, Brune M, Raimond J M and Haroche S 2006 quant-ph/0612138

Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction

Generation of any superposition of coherent states along a straight line via resonant atom－cavity interaction

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