Titlebook: Optical Resonators; Fundamentals, Advanc Norman Hodgson,Horst Weber Book 19971st edition Springer-Verlag London 1997 Polarisation.diffracti

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书目名称Optical Resonators影响因子(影响力)




书目名称Optical Resonators影响因子(影响力)学科排名




书目名称Optical Resonators网络公开度




书目名称Optical Resonators网络公开度学科排名




书目名称Optical Resonators被引频次




书目名称Optical Resonators被引频次学科排名




书目名称Optical Resonators年度引用




书目名称Optical Resonators年度引用学科排名




书目名称Optical Resonators读者反馈




书目名称Optical Resonators读者反馈学科排名

DOSE

dry-eye

Formidable

Unstable Resonatorsmisalignment as compared to stable resonators. In fact, unstable resonators are generally less sensitive to mirror tilt than stable resonators in fundamental mode operation. By using the equivalent G-parameter .=. . . .- . we can characterize the different resonator schemes as follows:

fledged

Wave Opticsation of light is obtained by utilizing Maxwell’s equations to derive the wave equations for the electric and the magnetic fields. If we neglect the vector properties of the field, the wave equation for the electric field . in homogeneous, isotropic, loss-free, dielectric media reads [1.1,1.3,1.40]: . with . being the speed of light in the medium.

合群

Polarizationese properties are called unpolarized. In the following we discuss completely polarized light which means that the electric field vector either points in a fixed direction or changes its orientation periodically.

Suppository

先锋派

Influence of Gain on Mode Structure and Losser resonator. In Part III we defined the mode radius . by using the second intensity moments. A first approximation, therefore, would be to use this mode radius for the definition of the mode cross section .. = π... For transverse multimode lasers this is a very good approach that provides output powers close to the observed ones.

FID

perimenopause

The Fabry Perot Resonatord laterally by means of apertures. Hence, for a given mirror spacing .. and a medium with index of refraction . between the mirrors, we will find steady state field distributions for all wavelengths λ. for which the following condition holds: . with: