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Download 3D Laser Microfabrication: Principles and Applications by Sami Franssila PDF

Posted On April 11, 2017 at 4:21 pm by / Comments Off on Download 3D Laser Microfabrication: Principles and Applications by Sami Franssila PDF

By Sami Franssila

A radical advent to 3D laser microfabrication know-how, top readers from the basics and idea to its a variety of effective functions, akin to the iteration of tiny gadgets or 3-dimensional buildings in the bulk of obvious materials.The booklet additionally offers new theoretical fabric on dielectric breakdown, permitting a greater figuring out of the variations among optical harm on surfaces and contained in the bulk, in addition to a glance into the future.Chemists, physicists, fabrics scientists and engineers will locate this a invaluable resource of interdisciplinary wisdom within the box of laser optics and nanotechnology.

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Couairon, M. Franko, B. Lamouroux, B. Prade, S. Tzortzakis and A. Mysyrovicz, Femtosecond laserInduced Damage and Filamentary Propa- 32 33 34 35 36 37 38 39 40 gation in Fused silica, Phys. Rev. , 89, 186601-1 (2002). W. B. M. D. G. Demos, Localized dynamics during laser-induced damage in optical materials, Phys. Rev. , 92, 087401-1 (2004). J. R. Oppenheimer, Three notes on the quantum theory of a periodic effect, Phys. , 31, 66 (1928). V. Keldysh, Ionization in the field of a strong electro-magnetic wave, Sov.

1 Schematic diagram of beams being refracted on an interface between two media: (a) n1 > n2 and (b) n1 < n2. 1 Three-dimensional Indensity Point-spread Function in the Second Medium before the geometrical focus. For n1 < n2 (see Fig. 1b), the traveling speed of the wavefront after refraction on the interface is slower than it is before refraction. Finally, the diffraction focus is located beyond the geometrical focus. It can be seen that rays with different angles of incidence are focused at different positions on the axis.

For n1 < n2 (see Fig. 1b), the traveling speed of the wavefront after refraction on the interface is slower than it is before refraction. Finally, the diffraction focus is located beyond the geometrical focus. It can be seen that rays with different angles of incidence are focused at different positions on the axis. This feature implies that the diffraction light distribution is enlarged along the axial direction. A high-NA objective suffers from more distortion than does a low-NA one. This aberration function depends on the focus depth d, the refractive indices, the excitation wavelength and the angle of convergence of a ray, and can be written as [11, 12] Uðh1 ; h2 ; dÞ ¼ Àkdðn1 cosh1 À n2 cosh2 Þ (1) where h1 and h2 denote the angles of incidence and refraction, respectively, and are linked by Snell’s law.

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