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By Nick Herbert

This in actual fact defined layman's advent to quantum physics is an available expedition into metaphysics and the that means of fact. Herbert exposes the quantum global and the clinical and philosophical controversy approximately its interpretation.

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Gatti and E. Brambilla, J. Opt. B: Quant. Semiclass. Opt. 4, S176 (2002), and references therein. 44 A. Gatti, E. Brambilla, O. Jedrkiewicz, and L. A. Lugiato 14. D. V. Strekalov, A. V. Sergienko, D. N. Klyshko, and Y. H. Shih, Phys. Rev. Lett. 74, 3600 (1995). 15. F. Ferri, D. Magatti, A. Gatti, M. Bache, E. Brambilla, and L. A. Lugiato Phys. Rev. Lett. 94, 183602 (2005). 16. R. S. Bennink, S. J. Bentley, and R. W. Boyd, Phys. Rev. Lett. 89, 113601 (2002). 17. W. A. T. Nogueira, S. P. Walborn, S.

34) In the experiment these averages are evaluated as spatial averages performed over the set of equivalent symmetrical pixel-pairs contained in the chosen sample regions, on which the mean photon number distribution is nearly uniform (see Fig. 8a,c). Each single shot of the laser provides a different ensemble, characterized by its pixel-pair average pe number ns + ni , in turn related to the parametric gain. In the experiment, ensembles corresponding to different gains are obtained by varying the pump-pulse energy.

32) , where, as we said, we ignore the frequency variable Ω. 33) 2 Spatial Entanglement in Optical Parametric Down-Conversion 25 where |n, x is the Fock state with n photons at point x. In this limit, there is ideally a perfect correlation in the number of signal–idler photons at the same near-field position (position entanglement). 3 Near- and Far-Field Correlations: Numerical Results in the General Case We now present the results obtained from the numerical model that includes the effects of the finite pump.

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