Titlebook: Instabilities and Chaos in Quantum Optics II; N. B. Abraham,F. T. Arecchi,L. A. Lugiato Book 1988 Springer Science+Business Media New York

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書(shū)目名稱(chēng)Instabilities and Chaos in Quantum Optics II影響因子(影響力)




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書(shū)目名稱(chēng)Instabilities and Chaos in Quantum Optics II被引頻次




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書(shū)目名稱(chēng)Instabilities and Chaos in Quantum Optics II讀者反饋




書(shū)目名稱(chēng)Instabilities and Chaos in Quantum Optics II讀者反饋學(xué)科排名

Obstruction

Theory and Experiments in the Laser with Saturable Absorberbsorbers are performed quite often for metrological or spectroscopical applications, and instabilities in the laser operation produced by intracavity saturable absorbers were observed very early in the development of laser systems.

卜聞

induct

Instabilities in Passive Optical Systems: Temporal and Spatial Patternsincluding phenomena that are quite similar in character to those found in laser systems.. Following the trail of the “classic” laser instabilities discovered in the early 1960’s., many instabilities of the “passive” type have also been uncovered and analyzed in great detail..

fluoroscopy

Experimental Studies of Instabilities and Chaos in Single-Mode, Inhomogeneously Broadened Gas Lasersin terms of gain and dispersion for many steady-state (and some simple time-dependent) behaviors in the interaction between fields and the material. This makes qualitative discussions of the physics of these devices not only possible but instructive..

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Extemporize

Book 1988tum Optics", held at the "Il Ciocco" Conference Center, Castelvecchio Pascoli, Lucca, Italy, June 28-July 7, 1987. The title of the volume is designated Instabilities and Chaos in Quantum Optics II, because of the nearly coincident publication of a collection of articles on research in this field ed

Commission

Shil’nikov Chaos in Lasersose dynamics is ruled by a low number of coupled variables. In the examined cases, experiments and theoretical model are in close agreement. In particular I describe Shil’nikov chaos, how it can be characterized, and the strong resulting coupling between nonlinear dynamics and statistical mechanics.

aspect

Instabilities in Fir Laserse in the active medium, γ. the population decay time in the active mediums, (γ+1) the pumping rate, normalized to 1 at laser threshold, E, P, D denote laser field; polarization and inversion in the active medium resp.

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