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Entanglement between collective fields via atomic coherence effects

Source: Phys. Rev. A 81, 013811 (2010); doi:10.1103/PhysRevA.81.013811

Published 19 January 2010

PACS
  • 42.50.Dv
    Quantum state engineering and measurements (quantum optics)
  • 42.50.Lc
    Quantum fluctuations, quantum noise, and quantum jumps (quantum optics)
  • 03.65.Ud
    Entanglement and quantum nonlocality
  • 03.67.Bg
    Entanglement production and manipulation (quantum information)
  • YEAR: 2010
PUBLICATION DATA
Publisher:
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Xiu Zhang1,2 and Xiangming Hu1
1Department of Physics, Huazhong Normal University, Wuhan 430079, People's Republic of China
2Department of Physics, Xiaogan University, Xiaogan 432000, People's Republic of China

We explore the quantum entanglement between two collective fields via atomic coherence effects. For three-level atoms in V configuration driven by two applied fields on two-photon resonance, one coherent superposition of the excited states is not excited, which is the counterpart of coherent population trapping. The coherence-induced depopulation makes two cavity fields in each collection combine into a quantum-beat, i.e., equivalently, the difference mode of the two components decouples from the driven atoms. The two sum modes, when they are arranged in the four-wave mixinglike interactions, can be prepared in Einstein-Podolsky-Rosen entangled state. Correspondingly, any two individual fields from different collective modes are entangled with each other. Furthermore, the effects of thermal reservoir and laser linewidths are discussed, and a generalization is given to the case in which each quantum beat involves more than two modes. ©2010 The American Physical Society
History: Received 29 October 2009; published 19 January 2010
Permalink: http://link.aps.org/abstract/PRA/v81/e013811
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