Y. Zhang, N. Wolters , X.H. Zeng , J. Schubert , W. Zander , H. Soltner , H.R. Yi , M. Banzet , F. Rüders , A.I. Braginski
{"title":"77K共面谐振的Washer rf SQUID磁力计","authors":"Y. Zhang, N. Wolters , X.H. Zeng , J. Schubert , W. Zander , H. Soltner , H.R. Yi , M. Banzet , F. Rüders , A.I. Braginski","doi":"10.1016/S0964-1807(98)00083-0","DOIUrl":null,"url":null,"abstract":"<div><p>We have developed a novel coplanar resonator serving as a tank circuit for rf washer supercenductry quantum interference device (SQUID)s. Two coplanar lines surround flux concentrator washers. The SQUID, 2.5 or 3.5<!--> <!-->mm in diameter, is coupled to the concentrator in the flip-chip configuration. In these layouts, the adjustable resonant frequency is up to the GHz-range. With SQUID loops of 10×500<!--> <em>μ</em>m<sup>2</sup> (SQUID inductance <em>L</em><sub>s</sub>=260 pH), we measured at 77<!--> <!-->K white flux noise levels <em>S</em><sub><em>φ</em></sub><sup>1/2</sup> of 8.5 <em>μφ</em><sub>0</sub>/√Hz. This corresponded to an energy resolution ϵ of 850<!--> <!-->h and a field resolution of about 16 fT/√Hz for a concentrator diameter of 13.4<!--> <!-->mm.</p></div>","PeriodicalId":100110,"journal":{"name":"Applied Superconductivity","volume":"6 7","pages":"Pages 385-390"},"PeriodicalIF":0.0000,"publicationDate":"1998-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0964-1807(98)00083-0","citationCount":"30","resultStr":"{\"title\":\"Washer rf SQUID Magnetometers with Coplanar Resonators at 77K\",\"authors\":\"Y. Zhang, N. Wolters , X.H. Zeng , J. Schubert , W. Zander , H. Soltner , H.R. Yi , M. Banzet , F. Rüders , A.I. Braginski\",\"doi\":\"10.1016/S0964-1807(98)00083-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>We have developed a novel coplanar resonator serving as a tank circuit for rf washer supercenductry quantum interference device (SQUID)s. Two coplanar lines surround flux concentrator washers. The SQUID, 2.5 or 3.5<!--> <!-->mm in diameter, is coupled to the concentrator in the flip-chip configuration. In these layouts, the adjustable resonant frequency is up to the GHz-range. With SQUID loops of 10×500<!--> <em>μ</em>m<sup>2</sup> (SQUID inductance <em>L</em><sub>s</sub>=260 pH), we measured at 77<!--> <!-->K white flux noise levels <em>S</em><sub><em>φ</em></sub><sup>1/2</sup> of 8.5 <em>μφ</em><sub>0</sub>/√Hz. This corresponded to an energy resolution ϵ of 850<!--> <!-->h and a field resolution of about 16 fT/√Hz for a concentrator diameter of 13.4<!--> <!-->mm.</p></div>\",\"PeriodicalId\":100110,\"journal\":{\"name\":\"Applied Superconductivity\",\"volume\":\"6 7\",\"pages\":\"Pages 385-390\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1998-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1016/S0964-1807(98)00083-0\",\"citationCount\":\"30\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Applied Superconductivity\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0964180798000830\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0964180798000830","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Washer rf SQUID Magnetometers with Coplanar Resonators at 77K
We have developed a novel coplanar resonator serving as a tank circuit for rf washer supercenductry quantum interference device (SQUID)s. Two coplanar lines surround flux concentrator washers. The SQUID, 2.5 or 3.5 mm in diameter, is coupled to the concentrator in the flip-chip configuration. In these layouts, the adjustable resonant frequency is up to the GHz-range. With SQUID loops of 10×500 μm2 (SQUID inductance Ls=260 pH), we measured at 77 K white flux noise levels Sφ1/2 of 8.5 μφ0/√Hz. This corresponded to an energy resolution ϵ of 850 h and a field resolution of about 16 fT/√Hz for a concentrator diameter of 13.4 mm.
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