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2. Non-separable beam generation |
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The previous experiment produces two squeezed modes with orthogonal polarizations, meaning that quantum correlations have been created between other polarization modes during the interaction with the atoms. We developed a general method to figure out the maximally entangled modes in the sense of the inseparability criterion for continuous variables recently derived by Duan et al. [1]. Using two homodyne detections, we have shown that the modes polarized at 45° with respect to the main linear polarizations are maximally entangled, and we have measured directly the "quadrature entanglement" of the beam exiting the cavity [2]. In a complementary experiment, we have mixed this beam with an intense coherent beam on a polarizing beamsplitter and obtained two spatially separated beams. By locking the intense beam phase with that of the entangled beam, we have mapped its entanglement onto a polarization basis, thus achieving "polarization entanglement" (i.e. entanglement between two pairs of Stokes operators [3]). |
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| Inseparability criterion for the maximally entangled modes, when the quadratures are rotated. Entanglement occurs when this value is less than 2. | ||
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[1] L.M. Duan, G. Giedke, J.I. Cirac, P. Zoller, Phys. Rev. Lett. 84, 2722 (2000) [quant-ph/9909044] [2] V. Josse, A. Dantan, A. Bramati, M. Pinard, E. Giacobino [quant-ph/0306147] [3] N. Korolkova, G. Leuchs, R. Loudon, T.C. Ralph, C. Silberhorn, Phys. Rev. A 65, 052306 (2003) [quant-ph/0108098] |
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