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Volumn 65, Issue 6, 2002, Pages

Perturbation theory for Maxwell’s equations with shifting material boundaries

Author keywords

[No Author keywords available]

Indexed keywords


EID: 84928785514     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.65.066611     Document Type: Article
Times cited : (110)

References (22)
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    • M. Skorobogatiy, M. Ibanescu, S. G. Johnson, O. Weisberg, T. D. Engeness, M. Soljačić, S. A. Jacobs, and T. Fink, J. Opt. Soc. Am. B (to be published).
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    • J. D. Joannopoulos, R. D. Meade, and J. N. Winn, Photonic Crystals: Molding the Flow of Light (Princeton University, Princeton, NJ, 1995).
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    • B. Z. Katsenelenbaum, L. Mercader del Río, M. Pereyaslavets, M. Sorolla Ayza, and M. Thumm, Theory of Nonuniform Waveguides: The Cross-Section Method (Inst. of Electrical Engineers, London, 1998).
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    • W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes in C: The Art of Scientific Computing, 2nd ed. (Cambridge University Press, Cambridge, 1992)
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    • G. B. Arfken and H. J. Weber, Mathematical Methods for Physicists, 5th ed. (Harcourt, San Diego, 2001)
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  • 20
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    • As yet another alternative, the waveguide-mode eigenproblem in terms of (Formula presented) yields a first-order correction that is a mixture between Eqs. (2) and (5) for different components of (Formula presented) 1 5 6
    • As yet another alternative, the waveguide-mode eigenproblem in terms of (Formula presented) yields a first-order correction that is a mixture between Eqs. (2) and (5) for different components of (Formula presented) 156.
  • 21
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    • Depending upon whether one is doing time- or z-(in)dependent perturbation/coupled-mode theory, there are additional (well known and easily derived) normalization factors multiplying the coupling integral 8 (see, e.g., Ref. 5
    • Depending upon whether one is doing time- or z-(in)dependent perturbation/coupled-mode theory, there are additional (well known and easily derived) normalization factors multiplying the coupling integral 8 (see, e.g., Ref. 5).
  • 22
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    • The exact power law would be at best (Formula presented), since this is the convergence rate of the eigenfrequencies 16, but is actually closer to (Formula presented) because of errors inherent in the numerical differentiation and the interpolated line integrals on a discrete grid
    • The exact power law would be at best (Formula presented), since this is the convergence rate of the eigenfrequencies 16, but is actually closer to (Formula presented) because of errors inherent in the numerical differentiation and the interpolated line integrals on a discrete grid.


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