1987
DOI: 10.1364/josaa.4.001289
|View full text |Cite
|
Sign up to set email alerts
|

Integral-equation formulation for scattering by dielectric discontinuities along open-boundary dielectric waveguides

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

0
4
0

Year Published

1993
1993
2001
2001

Publication Types

Select...
5

Relationship

0
5

Authors

Journals

citations
Cited by 12 publications
(4 citation statements)
references
References 20 publications
0
4
0
Order By: Relevance
“…The core half widths of waveguides 1 and 2 are d (1) and d (2), respectively, and the refractive indices of the core and cladding are nl = v/-5~, n2 = 1.0. Only fundamental TE0 mode is supported by the waveguide parameters mentioned above.…”
Section: Numerical Resultsmentioning
confidence: 99%
See 2 more Smart Citations
“…The core half widths of waveguides 1 and 2 are d (1) and d (2), respectively, and the refractive indices of the core and cladding are nl = v/-5~, n2 = 1.0. Only fundamental TE0 mode is supported by the waveguide parameters mentioned above.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Thus, a multi-layer PML medium with variable attenuation factor profile covered by a PEC backing is capable of simulating a reasonably reflectionless and absorptive medium, and lead to an improved boundary condition for FEM analysis of dielectric junction scattering problem, which requires an overall smaller problem domain than an ordinary PEC termination applied considerably farther away from the scatterer to attain the same numerical accuracy. Fig.3 shows the results concerning the reflection and transmission coefficients of the step dielectric waveguide as a function of step ratio d (1)/d (2) . The size of the computational domain is given by in L= x Lz = 8.0 x 1.0 in x and z direction.…”
Section: Numerical Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…')'P(•')ds' (80) where G is the dyadic Green's function for the problem. This formulation has been used extensively in scattering problems [Livernois and Nyquist, 1987;Sarkar et al, 1989] but has a major disadvantage in that it requires subsectioning of the cross section with a grid sufficiently fine with respect to the wavelength. Thus it becomes numerically intensive as the frequency increases or in the case of three-dimensional problems.…”
Section: Waveguiding Structuresmentioning
confidence: 99%