Trends in Electromagnetism - From Fundamentals to Applications 2012
DOI: 10.5772/34589
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Waveguides, Resonant Cavities, Optical Fibers and Their Quantum Counterparts

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Cited by 5 publications
(8 citation statements)
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“…Using the analogy between the movement of electrons in time-independent potentials and propagation of electromagnetic waves in dielectrics or metallic wave guides [18], mathematically, they are identical Sturm-Liouville problems; our results can be extended to several problems of electromagnetism and optics. This analogy can be easily developed for planar dielectric waveguides, namely, for "step-index" dielectrics, consisting of a slab of higher refractive index (core), sandwiched between two half spaces of lower refractive index (cladding).…”
Section: Discussionmentioning
confidence: 87%
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“…Using the analogy between the movement of electrons in time-independent potentials and propagation of electromagnetic waves in dielectrics or metallic wave guides [18], mathematically, they are identical Sturm-Liouville problems; our results can be extended to several problems of electromagnetism and optics. This analogy can be easily developed for planar dielectric waveguides, namely, for "step-index" dielectrics, consisting of a slab of higher refractive index (core), sandwiched between two half spaces of lower refractive index (cladding).…”
Section: Discussionmentioning
confidence: 87%
“…Graphical solutions are proposed by Guest [16], who made visible the similarities between the bound-state energies in a finite well and the modes of a metallic wave guide ( [17]; fig. (8.14)); actually, both the electrodynamic and quantum mechanical problems are equivalent forms of the same Sturm-Liouville problem [18]. Aronstein and Stroud [19] wrote the eigenvalue equation as…”
Section: Solving the Eigenvalue Equation Of The Finite Well: A Histormentioning
confidence: 99%
“…the energy of the bound states, are negative, which corresponds to the usual convention adopted in quantum mechanics. However, the form (30) of the potential has the advantage -also mentioned previously -that its levels become, in the limit of a very deep well, the levels of the infinite well. It is indeed easy to see that, for n → ∞, so for very deep wells, the quantization condition for the wave vector becomes k n a ≃ nπ, so…”
Section: The Quantum Square Wellmentioning
confidence: 86%
“…Also, the energy levels of the semi-infinite well, corresponding to the limit U 0 → ∞ in (30), are given by:…”
Section: The Quantum Square Wellmentioning
confidence: 99%
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