By Oleksiy Shulika, Igor Sukhoivanov
The booklet offers a mix of utilized and primary learn reflecting a number of subject matters in laser physics and applications
It offers either the review-type contributions and good researched and documented case reviews, and is meant for graduate scholars, younger scientist, and emeritus scientist working/studying in laser physics, optoelectronics, optics, photonics, and adjoining areas
The booklet comprises either experimental and theoretical stories, in addition to their combos of those two
Contains over a hundred thirty illustrations
Read Online or Download Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science PDF
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Additional info for Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science
A. 25 (5), 1169–1173 (2008) 22. : An assessment of coherent coupling through radiation fields in time varying slab waveguides. Opt. Quant. Electron. 39 (7), 533–551 (2007) 23. , Benson, T. : Whispering gallery mode transformation in a switched micro-cavity with concentric ring geometry. Opt. Quant. Electron. 40 (11–12), 818–820 (2008) 24. : Near field pattern images in 2D circular resonator with time varying plasma. IEEE Trans. Plasma Sci. 36 (4), 1222–1223 (2008) 25. : Frequency conversion and field pattern rotation in WGM resonator with transient inclusion.
As a results, an outgoing radiation may be multi-periodic or quasichaotic and may contain well-correlated or weakly connected spectral components. As a whole, the radiation may have various spectral and correlation features, and its dynamical properties are defined mainly by the so-called collective spontaneous emission of active centers [12, 47]. Sometimes CW lasers of this type are called “superradiant” ones, though in general case their proper name is “the class D lasers” [6, 28]. Indeed, a short temporal scale (< T2 ) in their dynamics and/or fluctuations [8, 17, 31], which is intrinsic to SR phenomenon, is absent in some cases.
5 Summary Wavelength tunable lasers based on MMI devices represent a technology that can significantly enhance the development of a broad range of tunable fiber lasers. Regardless of their simplicity and cost-effectiveness they are capable of providing large wavelength tuning ranges on the order of 90 nm using a single MMI filter. Current tuning schemes rely on moving elements, either mechanically moving a fiber or 32 D. A. -Arrioja et al. changing the liquid level, which for some applications can be a limiting factor.