Titlebook: Coherence and Quantum Optics VII; Proceedings of the S Joseph H. Eberly,Leonard Mandel,Emil Wolf Conference proceedings 1996 Springer Scien

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Reconstruction of Wigner Functions on Different Observation Levels,set of the single observable measurements (the so called optical homodyne tomography [2,3]) or via a simultaneous measurement of two non-commuting observables (see for instance a concept of propensities as discussed by Wódkiewicz [4] and others [5,6]) The completely reconstructed Wigner function, or

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Characterizing the Quantum State of Matter Using Emission Tomography,e.[3] In many experiments, particularly those on atoms and molecules, the aim is to engineer a specific state. Control of the system at the quantum level is intended to initiate a dynamic which can subsequently lead to a desired conclusion; the favoring of a particular dissociation pathway in a mole

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Cavity QED, Entanglement and Mesoscopic Quantum Coherences,sion wavelength. In such a confined space, the field amplitude associated with vacuum fluctuations in a mode is large and the coupling of the atom with these fluctuations becomes very strong, leading to non-linear optical effects at a quite unusual scale. Manipulation of atom and field properties is

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Quantum Cryptography over 14 Km of Installed Optical Fiber,s. When sensitive information is transferred from place-to-place it becomes vulnerable to eavesdropping or tampering with potentially catastrophic consequences. Thus, two of the main goals of cryptography are: the encryption of a message to render it unintelligible to a third party; and authenticati

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Quantum Computation,ticular problem. A specification of this set of instruction is called an algorithm. Examples of algorithms are the procedures taught in elementary schools for adding and multiplying whole numbers; when these procedures are mechanically applied, they always yield the correct result for any pair of wh

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Photon Scattering from Atoms in an Atom Interferometer: Coherence Lost and Regained,cs. It is of special interest both because of the difficulty of incorporating the resulting coherence loss into Schrödinger’s equation describing system A and because of its relevance to understanding the measurement process in particular and the connection between quantum mechanics and classical me

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Fluctuating Casimir Forces and Mirror-Induced Radiation,ed by “broad-band” problems with a continuous spectrum of modes extending to arbitrarily high frequencies, even though the predicted end effects are far below the reach of experiments at present. Recently tackled questions of this kind concern the fluctuations of the zero-point forces experienced by

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Essence of Semiotic Engineering,e aforementioned field characteristics in PBG structures: (a) quantum states preparation via nonadiabatic periodic transitions, (b) pump-mode Fock-state generation, (c) lasing without inversion — atomic coherence by spontaneous decay, (d) two-atom interactions, and (e) near-resonant gap solitons and optical “excitons”.

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Medical Semiology and Linguistic Semiologyon statistics.[1] Its QE can approach 100%, while maintaining high number resolution (can distinguish between .(.) and .(. +1)), as well as sub-picosecond temporal resolution and single-mode spatial discrimination. In addition, it provides simultaneous temporal and spectral resolution. [2]