By Oleksiy Shulika, Igor Sukhoivanov
The publication offers 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 experiences, and is meant for graduate scholars, younger scientist, and emeritus scientist working/studying in laser physics, optoelectronics, optics, photonics, and adjoining areas
The booklet includes either experimental and theoretical experiences, in addition to their combos of those two
Contains over a hundred thirty illustrations
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Extra resources for Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science
19) m here bm = Hm(2) (k0 a)/Jm (n1 k0 a), k0 = ω0 /c, ω0 is complex eigenfrequency that can be found from the following dispersion equation (2) n1 Jm (n1 k0 a)H (2) m (k0 a) − J m (n1 k0 a)Hm (n1 k0 a) = 0. 20) ∗ The time dependence is assumed to be eiω0 (t−t ) (t −t ∗ ), where t ∗ < 0 is the moment of switching on the mode. The prime here represent differentiation with respect to the argument. At zero moment of time the refractive index of the resonator material changes in value from n1 to n2 in response to an external force.
If a mirror is placed at this free-space location where this self-image point occurs, the light will be reflected back into the MMF and the operating wavelength will be coupled back to the input SMF fiber. Since the selfimage position is wavelength dependent, by changing the position of the mirror along the MMF axis we can control the MMI peak transmission wavelength. Therefore, this effect can be used to select a specific wavelength from a broad spectrum by simple changing the position of the mirror.
631, T1 = 200) 3 Whispering Gallery Mode Microdisk Resonator with Dynamic Material Properties Fig. 6 Time dependence of the refractive index n(t ) n2 45 ... n1 t1 t 2 t1 + t2 these modes on the interval of media parameters relaxation after packet of N disturbing pulses for different values of t1 . 631. For the same modulation frequency it is possible to observe amplitude growth or decay depending on the ratio t1 /t2 and n1 /n2 . g. ). However we have to stress different vertical scales in Fig.
Advanced Lasers: Laser Physics and Technology for Applied and Fundamental Science by Oleksiy Shulika, Igor Sukhoivanov