Effective scheme for generating cluster states in optical cavity QED

2008 ◽  
Vol 372 (8) ◽  
pp. 1185-1189 ◽  
Author(s):  
Huai-Zhi Wu ◽  
Zhen-Biao Yang ◽  
Shi-Biao Zheng
2007 ◽  
Vol 24 (11) ◽  
pp. 3055-3058 ◽  
Author(s):  
Wu Huai-Zhi ◽  
Yang Zhen-Biao ◽  
Zheng Shi-Biao

2009 ◽  
Vol 48 (9) ◽  
pp. 2685-2691 ◽  
Author(s):  
Deng-Yu Zhang ◽  
Shi-Qing Tang ◽  
Li-Jun Xie ◽  
Xiao-Gui Zhan ◽  
Kai-Ming You ◽  
...  

Author(s):  
G. REMPE ◽  
T. FISCHER ◽  
P. MAUNZ ◽  
P. W. H. PINKSE ◽  
T. PUPPE

2011 ◽  
Vol 09 (supp01) ◽  
pp. 83-92 ◽  
Author(s):  
MATTEO BINA ◽  
FEDERICO CASAGRANDE ◽  
ALFREDO LULLI ◽  
MARCO G. GENONI ◽  
MATTEO G. A. PARIS

We describe the dynamics of tripartite state mapping and entanglement transfer from qubit-like radiation states to two-level atoms via optical cavity modes. When the entangled radiation is carried to the cavities by single-mode fibers, optimal pure and mixed state transfer is predicted for perfect mirror transmittance, and entanglement sudden death (and birth) is demonstrated for Werner input states. The general case of multi-mode fiber coupling is also discussed. The dynamics is finally investigated under various dissipative effects.


2015 ◽  
Vol 379 (38) ◽  
pp. 2291-2294 ◽  
Author(s):  
Dong Dong ◽  
Yan-Lei Zhang ◽  
Chang-Ling Zou ◽  
Xu-Bo Zou ◽  
Guang-Can Guo

2001 ◽  
Vol 56 (1-2) ◽  
pp. 108-116
Author(s):  
David Vitali ◽  
Giacomo Ciaramicoli ◽  
Paolo Tombesi

Abstract We study the possible limitations and sources of decoherence of a scheme for the deterministic generation of polarization-entangled photons based on an appropriately driven single atom trapped within an optical cavity. -Pacs: 03.67.Hk, 42.50.Gy, 32.80.Qk


2008 ◽  
Vol 19 (05) ◽  
pp. 741-747 ◽  
Author(s):  
WEN ZHANG ◽  
YI-MIN LIU ◽  
ZHANG-YIN WANG ◽  
ZHAN-JUN ZHANG

We propose a scheme for discriminating 16 mutually orthogonal 4-atom cluster entangled states (CES) via cavity QED in teleporting an arbitrary unknown two-atom state with a 4-atom CES as quantum channel. Utilizing the interaction of atoms with cavity and classical field, the complicated 4-atom CESs are transformed into the simple 4-atom product states. Hence the difficulty of measurement during the teleportation process is degraded. In the present scheme, we allow for the case of a strong classical driving field and the detuning between the atoms and the cavity is assumed large enough. Thereby the photon-number-dependent parts in the effective Hamiltonian can be neglected, and the scheme is insensitive to both the cavity decay and the thermal field.


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