Beam current sensor

Electricity: measuring and testing – Determining nonelectric properties by measuring electric... – Beam of atomic particles

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324127, 336225, 336229, 336DIG1, G01R 1900

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active

046879870

ABSTRACT:
A current sensor for measuring the DC component of a beam of charged particles employs a superconducting pick-up loop probe, with twisted superconducting leads in combination with a Superconducting Quantum Interference Device (SQUID) detector. The pick-up probe is in the form of a single-turn loop, or a cylindrical toroid, through which the beam is directed and within which a first magnetic flux is excluded by the Meisner effect. The SQUID detector acts as a flux-to-voltage converter in providing a current to the pick-up loop so as to establish a second magnetic flux within the electrode which nulls out the first magnetic flux. A feedback voltage within the SQUID detector represents the beam current of the particles which transit the pick-up loop. Meisner effect currents prevent changes in the magnetic field within the toroidal pick-up loop and produce a current signal independent of the beam's cross-section and its position within the toroid, while the combination of superconducting elements provides current measurement sensitivites in the nano-ampere range.

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Meservey, R., "Proposed Ammeter Using Flux Quantization", Journal of Applied Physics, vol. 39, No. 6, May 1968, pp. 2598-2605.
Tsubakihara, H., et al., "Specially Designed Cryostat for Measurement of Critical Current Density . . . ", Tech. Rep. Osaka Univ. (Japan), vol. 24, No. 1155-1190, Mar. 1974, pp. 37-41.
Harvey, I., "Cryogenic ac Josephson Effect emf Standard Using a Superconducting Current Comparator", Metrologia, vol. 12, No. 2, Dec. 1976, pp. 47-54.
Barbanera, S. et al., "A SQUID Device for ac Current Measurements . . . ", J. Appl. Phys., vol. 49, No. 2, Feb. 1978, pp. 905-909.
Pribory i Tekhnika Eksperimenta, No. 3, Flekkel, "A Meter for Measuring the Average Current in a Pulsed Beam . . . ", May-Jun. 1974, pp. 44-46.

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