Computational Nanophotonics: Modeling and Applications by Sarhan M. Musa

By Sarhan M. Musa

''Written in a fashion that's simply digestible to newcomers and valuable to pro execs, this publication introduces the main ideas of computational Finite distinction Time area (FDTD) procedure utilized in nanotechnology. It covers destiny functions of nanotechnology in technical in addition to new advancements and interdisciplinary study in engineering, technological know-how, and drugs. It comprises an summary of Read more...

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C. R. Doerr, Planar Lightwave Devices for WDM, Optical Fiber Telecommunications, Ed. I. Kaminow and T. , 2002. 3. A. Yariv and P. , 2007. P. K. Tien, R. Ulrich, and R. J. Martin, Modes of propagating light wave in thin deposited semiconductor films, Applied Physics Letters, 14, 291, 1969. J. T. Andrews, R. R. Kumar, and P. K. Sen, Prism coupling of light in optical waveguide, Proceedings of the COMSOL Conference 2010, Bangalore, India, 2010. 6. W. A. Pasmoou, P. A. Mandersloot, and M. K. Smit, Prism-coupling of light into narrow planar optical waveguide, Journal of Lightwave Technology, 7(1), 175–180, 1989.

1). Process gases are generally introduced and regulated by way of mass flow controllers, while metals such as Ga may be introduced either by organometallic precursors or by placing a metal pellet within the reactor. 1a). The diameter of the nanowire is generally determined by the size of the alloy droplet, which is determined by the original size of the metallic cluster. By using monodispersed metal nanocrystals, a narrow diameter distribution of nanowires can be achieved [79]. The application of conventional epitaxial crystal growth techniques to the VLS process is possible to gain precise orientation control during nanowire growth.

Although low scale of integration (LSI) has been used for the optimization of an optical power switch 1 · 2 coupler by using evolution strategies [21], variational optimization technique has been found to be more fast and efficient for a relatively simple problem of coupler optimization [22]. The 1 · 2 coupler optimization has now been extended to a more generic problem of 1 · 4 optical power splitter based on a multimode interference (MMI) coupler [23]. The GA used here optimizes the geometrical characteristics of the device in such a way so as to achieve the desired spatial interference of four simultaneous electric fields (modes) at the end face of the MMI, thereby producing equally splitting ratios.

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