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Design, Fabrication and Characterization of a Microwave Resonator ...

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2.1 The Coplanar Transmission LineFigure 2.5: Configuration <strong>of</strong> the dielectric capacitance <strong>of</strong> a CBCPW.for the calculation <strong>of</strong> C CPW (2.4).That means, the moduli <strong>of</strong> the dielectric <strong>and</strong> the air-filled regions are equal. The parameterq simplifies toq =which tends to 1 2for very large heights again.K(k)K(k ′ )K(k)K(k ′ ) + K(k , (2.8)1)K(k 1 ′ )2.1.2.3 Isotropy <strong>of</strong> the DielectricThe relative permittivity ε r (used in (2.4)) <strong>and</strong> the height <strong>of</strong> the substrate H (see e.g. (2.5))depend on the isotropy <strong>of</strong> the dielectric material.In this work Silicon <strong>and</strong> Sapphire are used as substrate materials.Silicon is an isotropic material with ε r = 11.9.For Sapphire one needs to replace the relative permittivity with an effective permittivityε r = √ ε x,z · ε y = 10.34with ε y = 11.5 (c-axis) <strong>and</strong> ε x,z = 9.3 (a,b-axis) according to [3].The height has to be replaced by√εx,zH e = · H = 0.9Hε y2.1.3 Summary <strong>of</strong> Capacitance CalculationsUsing C Air <strong>and</strong> C diel , as defined in the last subsections, the phase velocity v ph <strong>and</strong> the waveimpedance Z c can be calculated:v ph =Z c ==c 0√εe f f(2.9)1C CPW v ph=2 · √εe f f ·√εe f fc 0 C CPWZ 0(K(k)K(k ′ ) + K(k 1)K(k ′ 1 ) ) (2.10)7

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