By Edik U. Rafailov
During this monograph, the authors tackle the physics and engineering including the most recent achievements of effective and compact ultrafast lasers according to novel quantum-dot constructions and units. Their procedure incorporates a wide diversity of laser structures, whereas bearing in mind not just the actual and experimental features but in addition the a lot wanted modeling instruments, therefore supplying a holistic knowing of this scorching subject
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Additional resources for Ultrafast Lasers Based on Quantum Dot Structures: Physics and Devices
Example text
Edited by Rich P. Mildren and James R. Rabeau. © 2013 Wiley-VCH Verlag GmbH & Co. KGaA. Published 2013 by Wiley-VCH Verlag GmbH & Co. KGaA. 2 1 Intrinsic Optical Properties of Diamond also includes the dependence of optical properties on basic variables such as wavelength, temperature, and isotopic composition. Although the scope is limited to bulk intrinsic properties, the intention is to stimulate a further expansion of the knowledge base as the limits of measurement resolution and performance are extended, and as more detailed investigations emerge into areas such as surface optics, crystal variants, and nano-optical effects.
A) Raster scan obtained from the detection of all photons, displaying both FND and cell autofluorescence signals; (b) Time-gated raster scan constructed from photons detected at between 15 and 0 12×103 10 8 6 4 2 0 0 Counts/ 20 ms 800 (b) 25 20 15 10 5 0 counts/ 20 ms 1200 counts/ 20 ms 50 100 150 Time/ ns 200 53 ns after the laser excitation pulses; (c) Fluorescence lifetime decay curve from the FNDs shown in panel (a). The gray region is the time-delay range, in which the photons are excluded to build the time-gated raster scan in panel (b).
Combinations with greater confidence. 4, along with their suggested assignments of the likely critical point phonons. 06 µm (1975 cm−1) all correspond to phonons in the <110> symmetry direction, for which there is an “accidental” critical point in the dispersion curves for one or both of the phonons involved in the assigned combinations. 75 µm (>2665 cm−1); however, such a procedure is very difficult due to the greatly increased number of phonon combinations, the lack of detailed knowledge on transition probabilities, and the poor visibility of critical point locations.