Read e-book online Active Glass for Photonic Devices: Photoinduced Structures PDF
By Professor Kazuyuki Hirao, Dr. Tsuneo Mitsuyu, Dr. Jinhai Si, Dr. Jianrong Qiu (auth.), Professor Kazuyuki Hirao, Dr. Tsuneo Mitsuyu, Dr. Jinhai Si, Dr. Jianrong Qiu (eds.)
This ebook specializes in chosen issues that are new and of primary value within the program of lively glasses in photonic units. many of the chapters take care of glasses lower than the motion of upper electromagnetic fields, resembling these produced by way of femtosecond lasers. They hide the production and research of brought about constructions in glasses and a few sensible units utilizing energetic glasses. This booklet is designed for either graduate scholars and researchers within the field.
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Extra resources for Active Glass for Photonic Devices: Photoinduced Structures and Their Application
This means that ,elf becomes more important in the quasi-equilibrium state between the electron and phonon systems. In the time region T > 10 ps, therefore, both contributions to the nonlinear optical response should be considered. As will be discussed later, an increase in the phonon temperature plays an important role in ,elf over a long time scale. In contrast with the results found here, Perner et al. reported that ,elf in the Drude term is most effective for the nonlinear optical response in the gold nanoparticle system .
The inset shows the long-time-scale behavior. The temporal behavior is decomposed into two decay components, a fast decay component (less than 3 ps) and a slow decay component (more than 100 ps). It is suggested that the fast decay constant reflects the thermal equilibrium process between the electron system and lattice system in the metallic nanoparticle and the slow decay constant comes from the cooling process by thermal diffusion from the metallic nanoparticle to the host matrix [49, 54J. 8 and 120 ps by fitting.
A dispersionless d band and a parabolic conduction band with a gap energy liwg were assumed. 13) and al and b1 are Mie scattering coefficients . Here, Ro is the diameter of the nanoparticle, N is the number density of nanoparticles in the sample, c is the velocity of the light, and Cglass is the dielectric constant of the glass matrix. In Fig. 12) is shown as a dotted curve. 4. 5 K. 158 eV. The 22 1. 4. 7       dotted curve reproduces the absorption spectrum excellently.
Active Glass for Photonic Devices: Photoinduced Structures and Their Application by Professor Kazuyuki Hirao, Dr. Tsuneo Mitsuyu, Dr. Jinhai Si, Dr. Jianrong Qiu (auth.), Professor Kazuyuki Hirao, Dr. Tsuneo Mitsuyu, Dr. Jinhai Si, Dr. Jianrong Qiu (eds.)