By Alphan Sennaroglu
ISBN-10: 0849335892
ISBN-13: 9780849335891
As a result of the favorable features of solid-state lasers, they've got develop into the popular applicants for a variety of functions in technology and expertise, together with spectroscopy, atmospheric tracking, micromachining, and precision metrology. providing the latest advancements within the box, Solid-State Lasers and functions specializes in the layout and purposes of solid-state laser systems.
With contributions from prime foreign specialists, the booklet explores the most recent study effects and purposes of solid-state lasers in addition to a number of laser platforms. the start chapters speak about present advancements and purposes of recent solid-state achieve media in several wavelength areas, together with cerium-doped lasers within the ultraviolet diversity, ytterbium lasers close to 1µm, rare-earth ion-doped lasers within the eye-safe area, and tunable Cr2+:ZnSe lasers within the mid-infrared variety. the remainder chapters research particular modes of operation of solid-state laser structures, reminiscent of pulsed microchip lasers, high-power neodymium lasers, ultrafast solid-state lasers, amplification of femtosecond pulses with optical parametric amplifiers, and noise features of solid-state lasers.
Solid-State Lasers and purposes covers crucial facets of the sector to supply present, accomplished assurance of solid-state lasers.
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Additional info for Solid-state lasers and applications
Example text
When the pulse width of the laser is comparable to the thermalization times of the laser manifolds it is not possible to accurately calculate the peak output power of the laser pulses without accurately knowing the thermalization times. 30) is independent of the thermalization times. 18 and Nf is the population inversion well after the peak of the output pulse. 33) ⎤ ⎥ = 0. 35) Eo,max = and is obtained for where γrt,p = γrt – γo is the round-trip parasitic loss coefficient. For smaller values of αr optimization is easily performed numerically once the material parameters of the system are known.
The electrical field within the optical beam of a high-power laser can be large enough to damage optical components. This is particularly important in high-peak-intensity pulsed lasers such as passively Q-switched microchip lasers. 2 Cavity Designs One common feature of many applications for miniature lasers is that mode quality is at least as important as total power. As a result, miniature lasers are usually designed to operate in the fundamental transverse mode. Most of the results and formulas presented in this section are derived for fundamental-mode operation and may require some modification for lasers operating in multiple transverse modes.
One approach to minimize this limitation is to cw pump the Q-switched laser just below threshold and then quickly raise the pump power to its maximum value just before an output pulse is desired. This technique results in the greatest pulse-to-pulse timing stability. , 1996). These approaches have resulted in timing jitter as low as 65 ps (Hansson and Arvidsson, 2000), at the expense of added system complexity and some sacrifice in the amplitude and pulsewidth stability of a true passively Q-switched system.
Solid-state lasers and applications by Alphan Sennaroglu
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