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Characterization and optimization of entangled states produced by a self-phase-locked OPO J. Laurat, G. Keller, J.A.O. Huguenin T. Coudreau, N. Treps, C. Fabre Laboratoire Kastler Brossel, ENS, CNRS, UPMC
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20052 “Non-separables” states Intense beams : quadratures of the electromagnetic field Quantum information with intense beams Principes
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20053 Qualifying inseparability Inseparability L.M. Duan et al., C. Simon (PRL 2000) Measuring entanglement Frequency-degenerate operation required Entanglement $ Squeezing
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20054 Covariance matrix formalism Single-mode covariance matrix Covariance matrix and squeezing characterizes completely the state
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20055 Two-mode covariance matrix Measuring entanglement
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20056 Parametric down-conversion Triply resonant optical cavity Principle of OPOs OPO Principles
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20057 Specificities of OPOs Oscillation threshold Emission of intense, coherent beams Orthogonally-polarized beams (“type II” phase matching) Principles
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20058 Ensuring frequency-degenerate operation Signal and idler frequency difference “arbitrary” Synchronizing/phase-locking two oscillators Add a linear coupling Frequency & phase - locking of signal and idler SPL OPO Mason & Wong, Opt. Lett. (1998)
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 20059 Above threshold Simultaneous measurement of amplitude correlations and phase anti-correlations Above threshold Excess phase noise
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 200510 Below threshold – “Aligned” waveplate Measurement apparatus Measurement results Below threshold
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 200511 Below threshold – “aligned” waveplate Covariance matrix Inseparability Below threshold
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 200512 Below threshold – rotated waveplate Noise variances Covariance matrix Inseparability Below threshold
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 200513 Below threshold – maximizing entanglement Performing a non-local operation Inseparability Covariance matrix local oscillator
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 200514 Conclusions Self-Phase Locked OPO a good tool to produce entangled states Self-Phase Locked OPO a good tool to show the general properties of entangled states Polarization elements a good tool to manipulate entanglement
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Quantum Information Measuring Entanglement OPOs Optimizing entanglement Conclusions Perspectives Frisno 8, february 200515 Perspectives Working above threshold Full measurement of the covariance matrix Higher dimensions
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