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High-Frequency Resistance of Superconductors

Abstract

MEASUREMENTS by H. London1 on the heating of superconducting tin by high-frequency electromagnetic fields indicate the presence in the superconductor of some mechanism which enables it to absorb a measurable quantity of energy from the field provided the frequency is of the order of 1,000 Mc./sec. or more. Recent developments in radio technique have made it possible to employ a resonance method to investigate the effect, and this communication describes preliminary work at frequencies around 1,200 Mc./sec., corresponding to a free-space wave-length of 25 cm. The specimens were polycrystalline thin wires contained in quartz capillary tubes for rigidity, bent into a narrow U to form a twin transmission line roughly a quarter wave-length long, and surrounded, to eliminate radiation losses, by a cylindrical sheath, which was either silver-plated or lined with lead-foil to minimize resistive losses. Measurements of the width of the resonance curve of the system by a controlled variation of the oscillator frequency gave a value for the skin resistance of the specimen.

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References

  1. London, H., Proc. Roy. Soc., A, 176, 522 (1940).

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  2. Kamerlingh Onnes and Tuyn, “Intern. Crit. Tables”, 6, 124 (1929).

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  3. Appleyard, Bristow, London, H., and Misener, Proc. Roy. Soc., A, 172, 540 (1939).

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  4. Shoenberg, Proc. Roy. Soc., A, 175, 49 (1940).

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  5. Casimir, Leid. Comm., 261, c (1940).

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PIPPARD, A. High-Frequency Resistance of Superconductors. Nature 158, 234–235 (1946). https://doi.org/10.1038/158234c0

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