A Scheme for the Generation of Multi-Mode Schrodinger Cat States

[in Chinese]; [in Chinese]

[1] Guo G C, Zheng S B. Preparation ofentangled coherent states of the electromagnetic field based on detecting the state of theatom in the Jaynes-Cummings model [J]. Opt. Commun., 1997, 133:142～146

[4] Gerry C C. Proposal for a mesoscopic cavity QED realization of theGreenberger-Horne-Zeilinger state [J]. Phys. Rev. A., 1996, 54(4): &127;R2529～R2532

[5] Buzek V, Vidiclla-Barranco A, Knight P L. Superposition of coherent state:squeezing and dissipation [J]. Phys. Rev. A., 1992, 45(9): 6570～5214

[6] Gerry C C. Non-classical properties of even and odd coherent states [J]. J. Mod.Opt., 1993, 40(6): 1053～1071

[7] Brune M, Haroche S, Raimaid J M et al. Manipulation of photons in a cavity bydispersive atom-field coupling: Quantum-nondemolition measurements and generation ofschrodinger cat states [J]. Phys. Rev. A., 1992, 45(7):5193～5214

[8] Gerry C C. Generation of four-photon coherent states in dispersive cavity QED [J].Phys. Rev. A., 1996, 53(6):3818～3821

[9] Guo G C, Zheng S B. Generation of schrodinger cat states via the Jaynes-Cummingsmodel with large detuning [J]. Phys. Lett. A., 1996, 223:332～336

[10] Zheng S B, Guo G C. A method for generating schrodinger cat states withcontrollable components [J]. Opt. Commun., 1997, 138:317～319

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

[12] Ansari N A, Man'ko V. Phys. Rev. A., 1994, 50:1942