1997
DOI: 10.1109/77.621888
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Planar HTS gradiometers with large baseline

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Cited by 34 publications
(8 citation statements)
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“…All the dc SQUID-based gradiometers described above have the disadvantage that the SQUID itself has a nonzero response to magnetic field, producing an intrinsic imbalance. This problem is circumvented in the rf SQUID-based gradiometer by Zhang, Soltner, Krause et al (1997), resembling the configuration of Fig. 32(a), with a single, step-edge junction intersecting the central strip.…”
Section: B Gradiometric Flux Transformersmentioning
confidence: 99%
“…All the dc SQUID-based gradiometers described above have the disadvantage that the SQUID itself has a nonzero response to magnetic field, producing an intrinsic imbalance. This problem is circumvented in the rf SQUID-based gradiometer by Zhang, Soltner, Krause et al (1997), resembling the configuration of Fig. 32(a), with a single, step-edge junction intersecting the central strip.…”
Section: B Gradiometric Flux Transformersmentioning
confidence: 99%
“…The increase during movement may originate from sensor vibrations, from the motion of flux lines in the superconducting YBCO films, or from eddy currents generated in the copper by power line and other low-frequency fields. Recent work [7] with a new integration scheme, using a sapphire cold finger for planar rf gradiometers [14] operated with a Joule-Thomson cryocooler, demonstrates clearly that even during movement, the sensitivity ofthe SQUID is only weakly impaired. This leaves the last explanation as the most probable.…”
Section: Discussionmentioning
confidence: 99%
“…The YBCO HTS RF SQUID planar gradiometer was made by Julich SQUID Company (JSQ) [10]. Its baseline is 3.6 mm and the gradient field sensitivity is less than 1 pT 3.6 mm Hz at frequencies over 10 Hz.…”
Section: A Block Diagram Of the Saw-wave Eddy-current Ndementioning
confidence: 99%