The standard form of implementing a limited-diffusion light-beam emission method is the Cranks-Nixon method. The implementation of the transverse electric field TE is described by the optical radius propagation algorithm. Both FD-BPM and FD-MS analyzes use the approxima More
The standard form of implementing a limited-diffusion light-beam emission method is the Cranks-Nixon method. The implementation of the transverse electric field TE is described by the optical radius propagation algorithm. Both FD-BPM and FD-MS analyzes use the approximation of the waveguide structure and the optical field to a network of samples.
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AOD technology is very suitable for 2D optical performance. Recent studies have used imaging or holographic growth, called phase-contrast techniques, to create optical trap arrays. In general, for trap arrays, holographic technology may result in unusual transverse lase More
AOD technology is very suitable for 2D optical performance. Recent studies have used imaging or holographic growth, called phase-contrast techniques, to create optical trap arrays. In general, for trap arrays, holographic technology may result in unusual transverse laser modes. Be. The Lagour-Gaussian optical beam is one example of an unusual light emission mode that is described in this article.
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Our aim in this paper is to provide methods for obtaining the field distribution at the tip of a narrowed dual-core fiber. One of the most important of these methods is the finite difference method. To use the finite difference method, we have two analyzes, one is light More
Our aim in this paper is to provide methods for obtaining the field distribution at the tip of a narrowed dual-core fiber. One of the most important of these methods is the finite difference method. To use the finite difference method, we have two analyzes, one is light scattering analysis, both of which use Maxwell wave equations.
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