Conductor Loss Calculation of Coplanar Waveguide
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Waveguide Device Component
14 Figures and Tables
Fig. 3.1 : Diagram illustrating use of a conformal map to find the series impedance of a transmission line including the effect of finite resistance.
Fig. 3.10 : Comparison of predicted conductor losses with the extensive
Fig. 3.11 : Comparison of predicted conductor losses with the extensive
Fig. 3.12 : Calculated attenuation constant and effective series resistance (real part of series impedance) of a high Tc superconductor CPW. CPW dimensions are center conductor width 2a = 10 µm, gap b-a = 7 µm and ground plane width w
Fig. 3.2 : Diagram illustrating an example of scaling for a simple cylindrical wire.
Fig. 3.3 : Conformal mapping of a rectangular-shaped coplanar line based on Schwarz-Christoffel transformation (drawn not to scale).
Fig. 3.4 : Cross-sectional drawing of Coplanar waveguide; Half of center conductor width, a = 5 µm, gap between center conductor and ground plane, (b-a) = 7 µm,
Fig. 3.5(a) : Comparison between experimental and predicted results for attenuation constant with semi-insulating (SI) GaAs substrate.
Fig. 3.5(b) : Comparison between experimental and predicted results for attenuation constant with pyrex substrate.
Fig. 3.6(a) : Comparison between experimental and predicted results for effective index of refraction (neff) with semi-insulating (SI) GaAs substrate.
Fig. 3.6(b) : Comparison between experimental and predicted results for effective index of refraction (neff) with pyrex substrate.
Fig. 3.7 : Variation of series resistance and series inductance with frequency for pyrex substrate.
Fig. 3.8 : Variation of series resistance and series inductance with frequency for semi-insulating GaAs substrate.
Fig. 3.9 : Comparison of conductor losses between experimental results and those calculated from other existing quasi-static techniques.
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