Acta Optica Sinica, Volume. 20, Issue 1, 51(2000)

Preparation of Two-Mode SU(2) Schr dinger Cat States via Atom-Cavity-Field Raman Interaction

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    References(17)

    [1] [1] Schrodinger E. Diegegenwa:rfige situation in der quantenmechanik. Naturwissenschaften,1935,23:807~812

    [2] [2] Yurke B, Stoler D. Generating quantum mechanical superposition of macroscopically distinguishable states via amplitude dispersion. Phys. Rev. Lett.,1986,57(1):13~16

    [3] [3] Xia Y, Guo G. Nonclassical properties of even and odd coherent states. Phys. Lett. (A), 1989, 136(6): 281~283

    [4] [4] Janszky J, Vinogradov A V. Squeezing via one-dimensional distribution of coherent states. Phys. Rev. Lett., 1990,64(23):2771~2774

    [5] [5] Foldesi I, Adam P, Janszky J. Antisymmetric straight line superposition of coherent states. Phys. Lett. (A),1993,173(2):97~100

    [6] [6] Brune M, Haroche S, Raimond J M et al.. Manipulation of photons in a cavity by dispersive atom-field coupling: Quantum-nondemolition measurement and generation of “Schr dingercat”states. Phys. Rev. (A), 1992, 45(7): 5193~5213

    [7] [7] Garraway B M, Sherman B, Moya-Cessa H et al.. Generation and detection of nonclassical field by conditional measurements following two-photon resonant interactions. Phys. Rev. (A),1994,49(1):525~547

    [8] [8] Davidovich L, Maali A, Brune M et al.. Quantum switches and nonlocal microwave fields. Phys. Rev. Lett., 1993,71(15):2360~2363

    [9] [9] Zheng S B, Guo G C. A method for generating Schr dinger cat states with controllable components. Opt. Commun., 1997,138(1):317~319

    [10] [10] Guo G C, Zheng S B. Generation of Schr dinger cat state via the Jaynes-Cummings model with large detuning. Phys. Lett. (A),1996,223(2):332~336

    [11] [11] Chai C. Two-mode nonclassical state via superpositions of two-mode coherent states. Phys. Rev. (A), 1992, 46(11):7187~7191

    [12] [12] Zheng S B, Guo G C. Preparation of correlated two-mode Schr dinger cat states via the atomic interference method. Opt. Commun., 1997,137(5):308~310

    [13] [13] Gerry C C, Grobe R. Two-mode SU(2) and SU(1,1) Schr dinger cat states. J. Mod. Opt., 1997,44(1):41~53

    [15] [15] Monroe C, Meekhof D M, King B E et al.. A “Schr dinger cat” superposition state of an atom. Science, 1996, 272(5265):1131~1136

    [16] [16] Wodkiewicz K, Eberly J H. Coherent states, squeezed fluctuations, and su(2) and su(1,1) groups in quantum-optics applications. J. Opt. Soc. Am. (B),1985,2(3):485~466

    [17] [17] Deb B, Gangopadhyay G, Ray D S. Generation of a class of arbitrary two-mode field states in a cavity. Phys. Rev. (A),1995,51(3):2651~2653

    [18] [18] Xu L, Zhang Z M. Modified effective Hamiltonian for degenerate Raman process. Z. Phys. (B), 1994, 95(4): 507~510

    CLP Journals

    [1] Lai Zhenjiang, Zhang Li, Liu Baoping, He Shufang. The Phase Properties of the Field in Atoms and Light Filed Coupling System with Phase Dissipation[J]. Acta Optica Sinica, 2010, 30(9): 2730

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    [in Chinese]. Preparation of Two-Mode SU(2) Schr dinger Cat States via Atom-Cavity-Field Raman Interaction[J]. Acta Optica Sinica, 2000, 20(1): 51

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    Paper Information

    Category: Quantum Optics

    Received: Jul. 21, 1998

    Accepted: --

    Published Online: Aug. 9, 2006

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