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edited by S. Meshkov (AIP Press, Melville, NY)
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For a very general demonstration that ∼ 1 MW is the minimum circulating power that is required to beat the standard quantum limit in a wide variety of QND interferometer designs, see V. B. Braginsky, M. L. Gorodetsky, F. Ya. Khalili, and K. S. Thorne, in Proceedings of the Third Edoardo Amaldi Meeting on Gravitational Waves, edited by S. Meshkov (AIP Press, Melville, NY, 2000), p. 180.
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Y. Chen (private communication).
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Chen, Y.1
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3643090362
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was only -4.3 dB, the inferred degree of squeezing was much larger: after making an absolute accounting for passive linear losses, these authors inferred a degree of squeezing corresponding to approximately -12 dB, which provides a benchmark for how well the basis nonlinear optical process of parametric down conversion conforms to simple theoretical models [31]. Somewhat more recently, E. S. Polzik, J. Carri, and J. H. Kimble, Appl. Phys. B: Photophys. Laser Chem. B55, 279 (1992),
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have recorded quantum noise reductions of -6 dB directly in the observed homodyne current. In this case the degree of squeezing was limited not by passive linear losses, but instead by nonlinear light induced absorption in the potassium niobate crystal used for parametric down conversion. Quite recently, K. Schneider, M. Lang, J. Mlynek, and S. Schiller, Opt. Express 2, 59 (1998),
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Equation (133) can be derived by the techniques used in Ref. [25]; see especially Eqs. (13)-(15) of [25].
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61
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33847401375
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note
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The experimental challenge simply to reach the SQL for mirror position is daunting. Two recent experiments that addressed this challenge with small masses but were impeded by thermal noise are reported in Refs. [42] and [43].
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