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Bulk-Wave Acousto-Optic Bragg Diffraction, is wide enough and the light incident upon it is at the appropriate angle, the diffraction which then takes place is most generally referred to as Bragg diffraction in analogy to the selective reflection of X rays by the lattice planes of crystals first described by W.H. Bragg in 1913. The ultrason

大氣層

,Optical Waveguides — Theory and Technology,vices. The zigzag and potential-well models are employed to explain the waveguiding condition, concepts of effective waveguide index and waveguide modes. The mode equation is derived and solved for the slab waveguide and approximate methods, including the effective-index technique, to analyze channe

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小口啜飲

Wideband Acousto-Optic Bragg Diffraction in LiNbO3 Waveguide and Applications,tment of wide-band AO Bragg diffraction in a planar LiNbO. waveguide, the resulting devices, and some potential applications is given. The sequence of presentation for the content of the Chapter now follows. First, the basic configuration and mechanisms for planar guided-wave AO Bragg diffraction fr

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Guided-Wave Acousto-Optic Interaction in a ZnO Thin Film on a Nonpiezoelectric Substrate,ics led to the extensive study of the Bragg diffraction of Guided Optical Waves (GOW) by Surface Acoustic Waves (SAW). Since . et al. [6.1] first demonstrated SAW-GOW deflectors and modulators, numerous experiments have been carried out on various thin-film configurations. An extensive list of refer

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Spectrum Analysis with Integrated Optics,. and . [7.1] first proposed the use of IO technology for one-dimensional analog optical processing. Coherent analog optical processors have not found wide application because of excessive size, cost and environmental susceptibility. At least for one-dimensional applications, IO technology may remov

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