1997
DOI: 10.1002/(sici)1520-6432(199701)80:1<18::aid-ecjb3>3.3.co;2-m
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A wide‐angle beam propagation method using a finite element scheme

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Cited by 3 publications
(8 citation statements)
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“…First, we test the paraxial formulation. The lowest order eigenmode is analyzed using the imaginary distance BPM [37]- [39], in which the effective index is calculated by the following equation [38]: (25) where . The effective-index error is defined as…”
Section: Numerical Resultsmentioning
confidence: 99%
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“…First, we test the paraxial formulation. The lowest order eigenmode is analyzed using the imaginary distance BPM [37]- [39], in which the effective index is calculated by the following equation [38]: (25) where . The effective-index error is defined as…”
Section: Numerical Resultsmentioning
confidence: 99%
“…The BPM's developed during the last two decades can be roughly categorized in terms of the discretization in the transverse direction, i.e., fast Fourier transform (FFT-BPM) [3], finite-difference (FD-BPM) [4]- [10], finite-element (FE-BPM) [11]- [14], and method of lines (Mol-BPM) [15]. In the FFT-BPM only a uniform grid is valid, while in the other BPM's a nonuniform grid [16]- [25] is allowed to improve computational efficiency or describe a waveguide configuration accurately. For a longitudinally invariant waveguide, a nonuniform grid has been applied to the FD-BPM [16], [17], [20].…”
Section: Introductionmentioning
confidence: 99%
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“…The configuration parameters of the coupled waveguides are taken to be the same as those investigated by the finite-element BPM [19], i.e., m, and m. The computation parameters are , except for ( m for ), and . Fig.…”
Section: Evaluation Of -Derivative Of the Refractive Indexmentioning
confidence: 99%