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 publication specializes in chosen themes that are new and of basic value within the software of lively glasses in photonic units. many of the chapters care for glasses less than the motion of upper electromagnetic fields, comparable to these produced through femtosecond lasers. They hide the construction and research of triggered buildings 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 info for Active Glass for Photonic Devices: Photoinduced Structures and Their Application

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9 shows the temporal change of ~OD at the peak of the surfaceplasmon band. 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.

L. ••• . • \• • t::. 0e ~Y clr 10 0 20 Delay Time (p ) Fig. 11. Temporal changes of ~8e and Dotted line: corresponds to the value of 1 ~/'eff, which are defined in the text. efficient than ,elf around T = O. Other parameters only affect details of the transient absorption spectrum. In the region T > 10 ps, both 8 e and ,elf contribute to the transient absorption spectrum. 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.

Concentrations of the organic solutions and the OKS and THG nonlinearities. The nonlinearities were calculated for 1 M concentration. 58 Solution DEANST HH-SBA X molecular length. In the case of carbon disulfide, the electronic contribution accounts for only ~ of the Kerr nonlinearity; however, in the solution of the long HH -SBA molecule, the electronic contribution is almost ~. Increasing molecular length yields larger n~B(OKS)/n2B(OKS) values. The molecular length dependence of the nonlinear property was further investigated in the DFWM experiment.

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