By Oleksiy Shulika, Igor Sukhoivanov
The e-book offers a mix of utilized and primary examine reflecting a number of themes in laser physics and applications
It provides either the review-type contributions and good researched and documented case experiences, and is meant for graduate scholars, younger scientist, and emeritus scientist working/studying in laser physics, optoelectronics, optics, photonics, and adjoining areas
The ebook includes either experimental and theoretical experiences, in addition to their combos of those two
Contains over one hundred thirty illustrations
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Extra resources for Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science
1 Introduction Optical resonators have been attracting increasing attention recently due to their potential in a variety of scientific and engineering applications including low-threshold lasers , ultra-small filters  and miniature biosensors [3, 4]. In the simplest cases, such resonators have the shape of a thin disk, a ring or a sphere. In the vicinity of a curved surface whispering gallery (WG) modes can be excited due to almost total internal reflection of the light. Quality (Q) factor of these oscillations are extremely high because light becomes trapped within the resonator.
29 (24), 2867–2869 (2004) 21. , Boriskina, S. : Test of the FDTD accuracy in the analysis of the scattering resonances associated with high-Q whispering-gallery modes of a circular cylinder. J. Opt. Soc. Am. 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.
This distance corresponds, as we explained before, to the position where the self-image is formed. An analytical solution can be obtained under the asymptotic formulation  by expressing the difference in the longitudinal propagation constants between two radial modes as a function of the MMF parameters (core RI and diameter) and the operating wavelength . Therefore, by expressing the operating wavelength as a function of all other terms, the following expression is obtained, λ0 = p 2 nMMF DMMF LMMF with p = 0, 1, 2, .
Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science by Oleksiy Shulika, Igor Sukhoivanov