2014
DOI: 10.1063/1.4856475
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Surface-resistance measurements using superconducting stripline resonators

Abstract: We present a method to measure the absolute surface resistance of conductive samples at a set of GHz frequencies with superconducting lead stripline resonators at temperatures 1 -6 K. The stripline structure can easily be applied for bulk samples and allows direct calculation of the surface resistance without the requirement of additional calibration measurements or sample reference points. We further describe a correction method to reduce experimental background on high-Q resonance modes by exploiting TEM-pro… Show more

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Cited by 33 publications
(72 citation statements)
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“…At frequencies deviating from the resonance frequency the transmission decreases rapidly, leading to a Lorentzian form of the transmission signal around resonance frequencies [58]. After correction of the data performed similar to [38], a fit of a Lorentzian with center frequency ν and full width at half maximum ∆ν is possible. This enables the calculation of the quality factor Q = ν/∆ν for any given resonance, defined as the ratio of power stored to power dissipated each cycle.…”
Section: Experimental Setup and Methodsmentioning
confidence: 99%
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“…At frequencies deviating from the resonance frequency the transmission decreases rapidly, leading to a Lorentzian form of the transmission signal around resonance frequencies [58]. After correction of the data performed similar to [38], a fit of a Lorentzian with center frequency ν and full width at half maximum ∆ν is possible. This enables the calculation of the quality factor Q = ν/∆ν for any given resonance, defined as the ratio of power stored to power dissipated each cycle.…”
Section: Experimental Setup and Methodsmentioning
confidence: 99%
“…depend on the applied microwave power, due to two-level fluctuators [15] whereas at very high powers there can be nonlinear behavior due to the superconductor [57]. For our experiments, we want the applied power to be high enough for good signal-to-noise ratio in the transmission measurement but yet well below the power range where our stripline resonators becomes non-linear, [38], and we eventually used an input power of −30 dBm.…”
Section: Experimental Setup and Methodsmentioning
confidence: 99%
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