Method and device for measuring super conducting film surface resistance
A surface resistance and superconducting thin film technology, applied in the field of electronics, can solve problems such as measurement errors
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example 1
[0083] Example 1: The metal cavity 1 is made of high-purity oxygen-free copper, with an inner diameter of 19.0mm. Dielectric cylinder A and dielectric cylinder B adopt sapphire dielectric, the cylinder diameters are 6.8mm and 6.0mm respectively, and the length is 4.0mm. The microwave coupling line is coupled with a semi-rigid coaxial cable coupling ring. Support ring 5 uses pure polytetrafluoroethylene. The test metal sample is a polished high-purity oxygen-free copper plate with a diameter of 50.8mm. During the test, the test device was directly placed in liquid nitrogen at a temperature of 77K.
[0084] According to the field distribution in the resonator, G can be calculated A = 292.56 and G B = 352.44. Q is measured using medium cylinder A and medium cylinder B respectively 0A =13233.6, Q 0B =14850.0, resonant frequency f A = 15.429GHz and f B =16.431GHz. From this we can calculate Q r =54959.96.
[0085] Surface resistance of high-purity oxygen-free copper plat...
example 2
[0086] Example 2: The test sample adopts Tl 2 Ba 2 CaCu 2 o X Superconducting thin film, 50.8mm in diameter. During the test, the test device was placed directly into liquid nitrogen.
[0087] Test results: at liquid nitrogen temperature (77K), Tl 2 Ba 2 CaCu 2 o X The surface resistance R of the superconducting thin film s (14.761GHz) = 0.688mΩ, R s (15.428GHz) = 0.761mΩ.
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