By Oleksiy Shulika, Igor Sukhoivanov
The ebook provides a mix of utilized and primary examine reflecting a number of themes 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 e-book comprises either experimental and theoretical experiences, in addition to their mixtures of those two
Contains over a hundred thirty illustrations
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Extra info for Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science
631 46 N. 465 x 10 4 Fig. 63, n2 = n1 + Δn, observation point is located near the rim. It is seen that such kind of modulation leads to variation of the field amplitude preserving spatial field distribution and frequency of the mode. Amplitude alternation can be enhanced by increasing the depth of modulation. Possible applications of this phenomenon include time control of persistence properties of photonic devises. In conclusion, this chapter presents an analytical formulation of the WG mode transformation due to the temporal change of the refractive index in a thin circular microdisk resonator.
One end of the optofluidically tunable MMI filter was spliced to the isolator while the other end was spliced to the input of the 10/90 fiber output coupler. 06 nm. The 90 % output arm is spliced to the input of the other isolator to close the ring cavity. 437 to obtain a tuning range close to 90 nm. As 2 Tunable Lasers Based on Multimode Interference Effects 31 Fig. 434 Fig. 13 a Schematic of the optofluidically tunable MMI BOA fiber laser and b Superimposed spectral response of the optofluidically tunable MMI BOA fiber laser shown in Fig.
The transition to a more usual frequency representation is made by substitution q = iω/c. So, by finding residues at singular points, we can estimate the contribution of each excited mode into the total field. 999 · 10−4 i (TT wave). 8 · 10−4 . 3 · 10−4 and 42 N. 246 8 0 50 100 0 Normalized time (T) 50 100 Fig. 7 · 10−4 , respectively. Other excited leaky modes give even smaller contribution into total field. Numerical simulation confirms that the integral along branch cut exhibits negligibly small contribution into total field as well.