Titlebook: Squeezed and Nonclassical Light; P. Tombesi,E. R. Pike Book 1989 Springer Science+Business Media New York 1989 Maser.development.future.in

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Pulsed Squeezed Light, light, this limit is imposed by the following properties of the nonlinear material used for the parametric process: 1) small nonlinear response, 2) linear losses, 3) insufficient laser pump power and 4) optical damage at high pump powers. Optical cavities have been used. to enhance the nonlinear in

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Squeezing Thermal Microwave Radiation,noise was observed. When operated at 0.1K, the amplifier exhibited an excess noise of 0.28 K referred to the amplifier’s input. This excess noise is less than the vacuum fluctuation noise at the input. The device can be operated in a nonchaotic mode with a signal gain of 9 dB.

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Classical and Quantum Statistics in Partition of Highly Degenerate Light,y situation, recently the attention of some theoretical physicists has been attracted by an interesting paradox which shows, in the context of light beam-splitting, the existence of a surprising conflict between the expectations of QED and those dictated by the indistinguishability property of the p

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The Effect of Measurement on Interference in Phase-Space,ned in terms of “interference in phase-space”.. In this paper the concept of phase-space interference will be developed in terms of the Q-function of quantum optics. While this approach is quite different to that of Schleich and Wheeler, the result is of course the same. The use of the Q-function pe

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Squeezing in Optical Bistability,l cavity and driven by a coherent incident field. This type of system is fundamental in quantum optics, and since the mid seventies has been the object of the extensive literature on . (OB) (see e.g. Ref.4). The squeezing problem in this system is studied in Refs. 5–14.