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One-Dimensional Confinement

  • M. K. Barnoski

Abstract

Consider the dielectric slab waveguide1 of thickness t illustrated in Fig. 1. The waveguide is assumed to be infinitely thick in the y dimension, therefore, ∂/∂y = 0. For TE modes the longitudinal components of the electric field Ez vanishes. Substitution of Ez = 0 and ∂/∂y = 0 into Equations 67 and 68 of Chapter I relating the transverse and longitudinal components results in the following field equations.

Keywords

Canyon Road Transverse Electric Slab Waveguide Natural Dispersion Dielectric Slab 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© University of California 1974

Authors and Affiliations

  • M. K. Barnoski
    • 1
  1. 1.Hughes Research LaboratoriesMalibuUSA

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