• Acta Optica Sinica
  • Vol. 18, Issue 8, 1050 (1998)
[in Chinese]1, [in Chinese]1、2, and [in Chinese]2
Author Affiliations
  • 1[in Chinese]
  • 2[in Chinese]
  • show less
    DOI: Cite this Article Set citation alerts
    [in Chinese], [in Chinese], [in Chinese]. Janynes-Cummings Model for a Single Trapped Ion[J]. Acta Optica Sinica, 1998, 18(8): 1050 Copy Citation Text show less
    References

    [1] H.-I. Yoo, J. H. Eberly. Dynamical theory of an atom with two or three levels interacting with quantized cavity fields. Phys. Rep., 1985, 118(5): 239~337

    [2] B. Buck, C. V. Sukumar. Exactly soluble model of atom-phonon coupling showing periodic decay and revival. Phys. Lett. (A), 1981, 81(2,3): 132~135

    [3] C. V. Sukumar, B. Buck. Multi-phonon generalization of the Jaynes-Cummings model. Phys. Lett. (A), 1981, 83(5): 211~213

    [4] S. J. D. Phoenix, P. L. Knight. Periodicity phase and entropy in model of two-phonon resonance. J. Opt. Soc. Am. (B), 1990, 7(1): 116~174

    [5] R. L. de Matos Filho, W. Vogel. Second-sideband laser cooling and nonclassical motion of trapped ions. Phys. Rev. (A), 1994, 50(3): R1988~R1991

    [6] C. C. Gerry, J. H. Eberly. Dynamics of a Raman coupled model interacting with two quantized cavity fields. Phys. Rev. (A), 1990, 42(11): 6805~6815

    [7] D. A. Cardimona, V. Kovanis, M. P. Sharma et al.. Quantum collapses and revivals in a nonlinear Jaynes-Commings model. Phys. Rev. (A), 1991, 43(7): 3710~3723

    [8] M. Alexanian, S. K. Bose. Unitary transformation and the dynamics of a three-levels atom interacting with two quantized field models. Phys. Rev. (A), 1995, 52(3): 2218~2224

    [9] Y. Wu. Effective Raman theory for a three-level atom in the Λ-configuration. Phys. Rev. (A), 1996, 54(2): 1586~1592

    [10] Y. Wu. Simple algebraic method to solve a coupled-channel cavity QED model. Phys. Rev. (A), 1996, 54(5): 4534~4543

    [11] X. X. Yang, Y. Wu, Y. J. Lee. Unified and standardized procedure to solve various nonlinear Jaynes-Cummings models. Phys. Rev. (A), 1997, 55: 4545~4551

    [12] C. K. Law, J. H. Eberly. Dynamics of a two-channel Raman-coupled cavity QED model. Phys. Rev. (A), 1993, 47(4): 3195~3201

    [13] Liwei Wang, R. R. Puri, J. H. Eberly. Coupled-channel cavity QED model & exact solutions. Phys. Rev. (A), 1992, 46(11): 7192~7209

    [14] D. M. Meekhof, C. Monore, B. E. King et al.. Generation of nonclassical motional states of a trappedatom. Phys. Rev. Lett., 1996, 76(11): 1796~1799

    [15] C. Monroe, D. M. Meekhof, B. E. King et al.. Resolved-sideband Raman cooling of a bound atom to the 3D zero-point energy. Phys. Rev. Lett., 1995, 75(2): 4011~4014

    [16] I. Marzoli, I. Cirac, R. Blatt et al.. Laser cooling of trapped three-level ions: Designing two-level systems for sideband cooling. Phys. Rev. (A), 1994, 49(4): 2771~2779

    [17] J. I. Cirac, P. Zoller. Quantum computations with cold trapped ions. Phys. Rev. Lett., 1995, 74(20): 4091~4097

    [18] C. Monroe, D. M. Meekhof, B. E. King et al.. Demonstration of a fundamental quantum logic gate. Phys. Rev. Lett., 1995, 75(25): 4714~4717

    [19] G. Q. Ge, Y. Wu, X. Luo et al.. Optical bistablity and lasing without inversion in a system of driven two-level atoms with incoherent injection. Phys. Rev. (A), 1995, 52(2): 1783~1786

    [20] G. Q. Ge, X. Luo, Y. Wu et al.. Atomic coherence and bistable lasers without inversion. Phys. Rev. (A), 1996, 54(2): 1604~1608

    [21] E. S. Fry, Xingfu Li, Dmitri Nikonov et al.. Atomic coherence effects within the sodium D1 line: Lasing without inversion via population trapping. Phys. Rev. Lett., 1993, 70(21): 3235~3238

    [22] V. E. VanderVeer, R. J. J. VanDiest, A. Donszelmann et al.. Experimental demonstration of light amplification without population inversion. Phys. Rev. Lett., 1993, 70(21): 3243~3246

    [23] J. Gao, C. Guo, Chuan Guo et al.. Observation of light amplification without population inversion in sodium. Opt. Commun., 1993, 93(5,6): 323~327

    [24] A. Imamolglu, S. E. Harris. Lasers without inversion interference of dressed lifetime-broadened states. Opt. Lett., 1989, 14(24): 1344~1346

    [25] M. O. Scully, S. Y. Zhu, A. Gavrielides. Degenerate quantum-beat laser: Lasing without inversion and inversion without lasing. Phys. Rev. Lett., 1989, 62(24): 2813~2816

    [26] G. S. Agarwal. Dressed-state lasers and masers. Phys. Rev. (A), 1990, 42(1): 686~688

    [27] L. M. Narducci et al.. Spectrum of spontaneous emission in a Fabry-Perot cavity: theeffects of atomic motion. Opt. Commun., 1992, 94(13): 66~70

    [28] Y. Zhu. Lasing without inversion in a closed three-level system. Phys. Rev. (A), 1992, 45(9): R6149~R6152

    [29] Y. Zhu. Lasing without or with inversion in a closed four-level system. Phys. Rev. (A), 1993, 47(1): 495~499

    [30] D. Meschede, H. Walther, G. Muller. One-atommaser. Phys. Rev. Lett., 1985, 54(6): 551~554

    [31] Fam Le Kien, Georg M. Meyer, Marlan O. Scully et al.. Two-mode micromaser operating on three-level atoms. Phys. Rev. (A), 1994, 49(2): 1367~1377

    [32] K. An, J. J. Childs, R. R. Dasari et al.. A laser with one atom in an optical resonator. Phys. Rev. Lett., 1994, 73(25): 3375~3378

    [33] C. D. Helon, G. J. Milburn. Measuring the vibrational energy of a trapped ion. Phys. Rev. (A), 1995, 52(6): 4755~4762

    [34] P. Filipowicz, J. Javanainen, P. Meystre et al.. Quantum and semiclassical steady states of a kicked cavity mode. J. Opt. Soc. Am. (B), 1987, 3(6): 906~910

    [35] M. Fleischhauer, W. P. Schleich. Revivals made simple: Poisson summation formula as a key to the revivals in the Jaynes-Cummings model. Phys. Rev. (A), 1993, 47(5): 4258~4269

    [36] S. E. Harris, J. E. Field, A. Imamoglu. Nonlinear optical processes using electromagnetically induced transparency. Phys. Rev. Lett., 1990, 64(10): 1107~1110

    [37] M. Xiao, Yong-qing Li, Shao-zheng Jin et al.. Measurement of dispersive properties of electromagnetically induced transparency in Rubidum atoms. Phys. Rev. Lett., 1995, 74(5): 666~669

    [38] S.-Y. Zhu, L. M. Narducci, M. O. Scully. Quantum-mechanical interference effects in the spontaneous-emission spectrum of a driven atom. Phys. Rev. (A), 1995, 52(6): 4791~4802

    [39] A. H. Toor, S.-Y. Zhu, M. S. Zubany. Quantum interference in the spectrum of a driven atom: Effects of pumping and phase fluctuations. Phys. Rev. (A), 1995, 52(6): 4803~4811

    [40] J. I. Cirac, R. Blatt, A. S. Parkins et al.. “Dark” squeezed states of the motion of a trapped ion. Phys. Rev. Lett., 1993, 70(5): 556~559

    [41] J. I. Cirac, A. S. Parkins, P. Zoller et al.. Preparations of fock states by observation of quantum jumps in an ion trap. Phys. Rev. Lett., 1993, 70(6): 762~765

    [42] J. I. Cirac, R. Blatt, A. S. Parkins et al.. Quantum collapse and revival in the motion of a single trapped ion. Phys. Rev. (A), 1994, 49(2): 1202~1207

    [43] J. I. Cirac, R. Blatt, P. Zoller et al.. Laser cooling of trapped ions in a standing wave. Phys. Rev. (A), 1992, 46(5): 2668~2681