Download e-book for iPad: Advanced Lasers: Laser Physics and Technology for Applied by Oleksiy Shulika, Igor Sukhoivanov

By Oleksiy Shulika, Igor Sukhoivanov

ISBN-10: 9401794804

ISBN-13: 9789401794800

ISBN-10: 9401794812

ISBN-13: 9789401794817

The publication offers a mix of utilized and primary learn reflecting a number of themes in laser physics and applications
It provides either the review-type contributions and good researched and documented case reports, and is meant for graduate scholars, younger scientist, and emeritus scientist working/studying in laser physics, optoelectronics, optics, photonics, and adjoining areas

The ebook comprises either experimental and theoretical reports, in addition to their combos of those two
Contains over one hundred thirty illustrations

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Extra info for Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science

Example text

3) that if the phase factor (βν − β1 )z is an exact multiple of 2π we obtain an exact replica of the input field. 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 [21] 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 [22]. 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, .

27) it is observed that, upon inversion to the time domain, the expressions corresponding to GI m (n2 qρ) and FK m (qρ) exhibit a time delay that can be expressed in terms of the unite Heaviside functions, (tc/n2 + ρ − a) and (ct − ρ + a), inside and outside of the resonator, respectively. 21) and exhibits the same wavenumber and shifted frequencies predicted from the abrupt change in the material parameters. It does not depend upon the boundary shape and depend only on relative change in refractive index.

2) for a No-Core MMF in air. The advantage of this tuning mechanism is that changes to the length of No-Core MMF, with and without liquid, exhibit a linear peak transmission wavelength response as a function of the liquid level. The slope of the response is controlled by the effective RI and diameter which is directly related to the RI of the liquid. 28 mm, which correspond to peak wavelengths of 1534, 1506, and 1472 nm respectively. 444 of the No-Core fiber. The liquid level was increased in steps of 10 mm and the MMI spectral response was acquired with the OSA at each step.

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Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science by Oleksiy Shulika, Igor Sukhoivanov

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