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Titlebook: Coherence and Quantum Optics VI; Proceedings of the S Joseph H. Eberly,Leonard Mandel,Emil Wolf Conference proceedings 1989 Plenum Press, N

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31#
發(fā)表于 2025-3-26 21:43:10 | 只看該作者
First Presentation of the Basic Concepts, role of fluctuations along the build-up with respect to the initial ones. A quest for a discrimination between fluctuations on the initial condition and those along the path led to a new observation method, based on the statistics of passage times at a given threshold ..
32#
發(fā)表于 2025-3-27 02:32:34 | 只看該作者
33#
發(fā)表于 2025-3-27 06:40:28 | 只看該作者
34#
發(fā)表于 2025-3-27 11:38:47 | 只看該作者
35#
發(fā)表于 2025-3-27 17:34:18 | 只看該作者
Coequalizers in categories of algebras,itions almost indistinguishably from the five-equation model for the single mode laser with a homogeneously broadened two-level medium [1] which is isomorphic to the complex Lorenz model [2]. Qualitative features found in the model such as instability thresholds, types of pulsations, inverse period
36#
發(fā)表于 2025-3-27 20:25:37 | 只看該作者
,Beschr?nkte analytische Funktionen,ic oscillator with quartic anharmonicity. This model can describe a number of situations. For example, it can describe a highly excited Rydberg atom making transitions between close lying levels. It also describes a field propagating in a Kerr medium having space inversion symmetry. We assume that t
37#
發(fā)表于 2025-3-27 22:07:53 | 只看該作者
38#
發(fā)表于 2025-3-28 06:06:21 | 只看該作者
39#
發(fā)表于 2025-3-28 09:49:44 | 只看該作者
Untersuchung im 21. bis 24. Lebensmonat,dia with a cubic nonlinearity: instabilities which are driven by coherent transverse interactions of large scale (the typical scale is ., were d is the beam width). In a light beam in free propagation, and in optical resonators with coherent layouts, transverse interactions are of nature of diffusio
40#
發(fā)表于 2025-3-28 11:47:32 | 只看該作者
Untersuchung im 21. bis 24. Lebensmonat,upling constant, and γ is the Einstein . coefficient, formally, the standrd theory of resonance fluorescence assumes the limit . → ∞, ./γ → 0, with the ratio of Rabi frequency to atomic linewidth .finite.
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