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

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2 Theoretical Description <strong>of</strong> a CPW <strong>Resonator</strong>2.3.5 Superconducting <strong>Resonator</strong>Finally, we will discuss the temperature dependencies <strong>of</strong> the resonance frequency <strong>and</strong> thequality factor <strong>of</strong> superconducting resonators.From (2.24) <strong>and</strong> (2.21) one can directly observe that superconductivity influences thephase velocity v ph through the kinetic inductance defined by (2.22). The kinetic inductancedepends on the temperature dependent London penetration depth λ L (see (2.23)). In Figure2.12 the temperature dependence <strong>of</strong> the resonance frequency is shown. One can see thatwith constant length the resonant frequency decreases with increasing temperature.Figure 2.12: Dependence <strong>of</strong> the resonance frequency calculated with the kinetic inductancemodel for the Yale design on Silicon <strong>and</strong> Sapphire for a fixed length<strong>of</strong> 8.991 mm.The quality factor Q is also temperature dependent, according to (2.32) it consists <strong>of</strong> thetemperature dependent quantities β <strong>and</strong> α. In Figure 2.13 the quality factor dependence ontemperature is shown for Silicon <strong>and</strong> Sapphire.For Silicon one obtains quality factors <strong>of</strong> around 260. In our measurements the qualityfactor is one order <strong>of</strong> magnitude or more larger. The reason for this mismatching qualitiescould be that at lower temperatures the loss tangent is much lower than 0.004 (see Table 2.2).A value <strong>of</strong> around 0.00007 gives better matching results.22

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