Preparation of the Atomic Entangled States with Controllable Weighting Factors

[in Chinese]

[1] Einstein A, Podolsky B, Rosen N. Can quantum-mechanical description of physical reality be considered complete Phys. Rev., 1935, 47(5):777～780

[2] Greenberger D M, Horne M, Zeilinger A. In: Bell’s Theorem, Quantum Theory, and Conceptions of the Universe, Kafatos M eds, Dordrecht: Kluwer Press, 1989. 195

[3] Bennett C H, Brassard G, Crepeau C et al.. Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels. Phys. Rev. Lett., 1993, 70(13):1895～1899

[4] Zheng S B, Guo G C. Teleportation of an unknown atomic state through the Raman atom-cavity-field interaction. Phys. Lett. (A), 1997, 232(2):171～174

[5] Phenix S J D, Barnett S M. Non-local interatomic correlations in the micromaser. J. Modern Opt., 1993, 40(6):979～983

[6] Kudryavtsev I K, Knight P L. Atomic entaglement and Bell’s inequality violation. J Modern Opt., 1993, 40(9):1673～1679

[7] Cirac J I, Zoller P. Preparation of macroscopic superpositions in many-atom system. Phys. Rev. (A), 1994, 50(4):R2799～R2802

[8] Song K H, Guo G C. Preparation of two-atom entangled states via the quantized cavity field resonant interaction with atom. Chinese J. Laser, 1999, 8(2):153～156

[9] Zheng S B, Guo G C. Preparation of multi-atom GHZ states. J. Modern Opt., 1997, 44(5):963～966

[10] Zheng S B, Guo G C. Generation of multi-atom entangled states via the Raman atom-cavity-field interaction. Chinese Phys. Lett., 1997, 14(7):485～487

[11] Song K H, Guo G C. Preparation of entangled atomic states via atoms interacting with the cavity-field in SU(1,1) coherent state. Chinese Phys. Lett., 1999, 16(3):161～162

[12] Gerry C C. Preparation of multiatom entangled states through dispersive atom-cavity-field interaction. Phys. Rev. (A), 1996, 53(4):2857～2860

[13] Braunstein S L, Mannand A, Revzen M. Maximal violation of Bell inequalities for mixed states. Phys. Rev. Lett., 1992, 68(1):3259～3261

[14] Holland M J, Walls D F, Zoller P. Quantum nondemolition measurements of photon number by atomic-beam deflection. Phys. Rev. Lett., 1991, 67(3):1716～1719

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

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

[17] Fregberger M. Simple example of nonlocality: atoms interacting with correlated quatized fields. Phys. Rev. (A), 1995, 51(4):3347～3350