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Titlebook: Optical Bistability; Charles M. Bowden,Mikael Ciftan,Hermann R. Robl Book 1981 Plenum Press, New York 1981 development.laser.physics.stabi

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发表于 2025-3-21 18:01:05 | 显示全部楼层 |阅读模式
书目名称Optical Bistability
编辑Charles M. Bowden,Mikael Ciftan,Hermann R. Robl
视频video
图书封面Titlebook: Optical Bistability;  Charles M. Bowden,Mikael Ciftan,Hermann R. Robl Book 1981 Plenum Press, New York 1981 development.laser.physics.stabi
描述During the past few decades we have witnessed at least two major innovations in science which have had substantial impact on technology as well as science itself, pervasive enough to modify many facets of our daily lives. We refer, of course, to the tran­ sistor and the laser. It is striking that now with the advent of optical bistability we may have opened the door to another such field, which combines these two aspects (transistor and laser) and has the possibility for important device applications as well as providing a unique window into the as yet not thoroughly explored frontiers of nonequilibrium statistical physics. This has prompted us to organize an international conference on the subject of optical bistability to provide an adequate means for assessing the current state of the art of this important field and to stimulate further significant developments by means of in­ tense technical exchange and interaction among the leading scien­ tists in this subject area.
出版日期Book 1981
关键词development; laser; physics; stability; statistical physics
版次1
doihttps://doi.org/10.1007/978-1-4684-3941-0
isbn_softcover978-1-4684-3943-4
isbn_ebook978-1-4684-3941-0
copyrightPlenum Press, New York 1981
The information of publication is updating

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Bistable Systems in Nonlinear Optics,osing an intracavity medium with a non-linear polarizability. As an example of a system with a second-order nonlinear susceptibility .. we consider sub/second harmonic generation and for a system with a third-order nonlinear susceptibility .. we consider a nonlinear dispersive medium such as Kerr li
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Optical Bistability Experiments and Mean Field Theories,d spherical-mirror Fabry-Perot cavity The conditions of large homogeneous broadening (due to high optical power and buffer gas broadening) allow us to interpret the experiments in terms of a two-state model for the D. transition. The experimental results, taken under conditions appropriate to the me
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Microwave Dispersive Bistability in a Confocal Fabry-Perot Microwave Cavity,r and absorber parameters by taking into account the spatially averaged absorption coefficient of the gas. The state equation so obtained exhibits a bistable behaviour. The transmittance of a microwave cavity filled with ammonia gas and tuned at the frequency of the (3,3) inversion line of ammonia i
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