tion predictions in heterogeneous urban environments with arbitrary building layouts and heights. The method is based on image theory, and has high computational efficiency compared to the precedent methods resorting to the ray-launching scheme. The presented hybrid method gives relatively accurate
Weak Guidance Modal Analysis and Dispersion Curves of an Infrared Lightguide Having a Core Cross Section with a New Type of Asymmetric Loop Boundary
✍ Scribed by Vivek Singh; B. Prasad; S.P. Ojha
- Publisher
- Elsevier Science
- Year
- 2000
- Tongue
- English
- Weight
- 112 KB
- Volume
- 6
- Category
- Article
- ISSN
- 1068-5200
No coin nor oath required. For personal study only.
✦ Synopsis
We make an analytical investigation of the modal characteristic equation of an infrared lightguide having a guiding region whose cross section has a Ž . new type of asymmetric loop boundary. We choose new coordinates , , z Ž . instead of r, , z , and assuming that the propagation is along the z direction, we use the boundary conditions under the weak guidance approximation to obtain the modal characteristic equation and cutoff equation. From the cutoff equation we get the number of modes propagated in the guiding region for a given size of the guiding region. From the characteristic equation the dispersion curves are obtained in the second telecommunication window at s 1.3 and 1.55 m. This analysis is applicable to dielectric 0 waveguides in the microwave region also.
📜 SIMILAR VOLUMES
## Abstract The purpose of this paper is to introduce a simple analytical technique based on scalar‐wave approximation to study the modal characteristics of a new lightguide having a lemniscate of Bernoulli‐type core cross section. This type of structure may be conceived as a practical situation wh
Using Goell's point-matching method under the weak guidance approximation, we obtain and interpret the modal dispersion cur¨es for some low-order modes sustained by an optical wa¨eguide whose guiding region has a double-con¨ex-lens-like cross section. It is found that the dispersion cur¨es are of th
Figure 7 Plots of the transmission ratio T versus the half-branching angle A for the AGI structure with different values of refractive index n of the PFA 3 and the AGI structures are 7.8 and 9.3Њ, respectively. The improvement in the angle is thus 1.5Њ. For still lower n , 3 further improvement woul