Nicholas J. Exon, Mark N. Keene, Julian S. Satchell, Nigel G. Chew, Matthew J. Wooliscroft, Karan Lander, Richard G. Humphreys
{"title":"A low noise HTS SQUID magnetometer with an on-chip pickup loop coupled via an intermediate flux transformer","authors":"Nicholas J. Exon, Mark N. Keene, Julian S. Satchell, Nigel G. Chew, Matthew J. Wooliscroft, Karan Lander, Richard G. Humphreys","doi":"10.1016/S0964-1807(99)00026-5","DOIUrl":null,"url":null,"abstract":"<div><p>For many SQUID applications robust, compact magnetometers are required with low flux noise and high effective area at 77<!--> <!-->K. Low flux noise is achieved by using a low inductance SQUID. A low inductance SQUID will also have a high transfer function, allowing simplified direct readout schemes to be used. For maximum field sensitivity the SQUID needs to be coupled to a pickup loop of large area and therefore large inductance. We have modelled, designed and fabricated a novel HTS magnetometer consisting of a low inductance (<16<!--> <!-->pH) dc SQUID coupled to a 28<!--> <!-->nH pickup loop flux transformer fabricated on the same 1<!--> <!-->cm<sup>2</sup> substrate. Efficient coupling was achieved by using a flip-chipped intermediate flux transformer. This configuration produces a magnetometer with a high sensitivity per unit area. The magnetometers incorporate PrBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub> isolation layers and two 2<!--> <em>μ</em>m diameter CAM variant junctions. Thick YBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub><span> layers were used to improve coupling and decrease the demagnetisation factor wherever possible. Our device had a transfer function of 913</span> <em>μ</em>V/<em>Φ</em><sub>0</sub> which allows direct readout without any matching or additional positive feedback arrangements. The measured effective area at 77<!--> <!-->K was 0.58<!--> <!-->mm<sup>2</sup> (3.6<!--> <!-->nT/<em>Φ</em><sub>0</sub>). The magnetometer white noise was 18<!--> <!-->fT/<span><math><mtext>Hz</mtext></math></span> and at 1<!--> <!-->Hz was 380<!--> <!-->fT/<span><math><mtext>Hz</mtext></math></span>. This was reduced at 1<!--> <!-->Hz to 120<!--> <!-->fT/<span><math><mtext>Hz</mtext></math></span> using bias reversal. The measured white noise was higher than the design value and is largely due to Johnson noise from the PrBa<sub>2</sub>Cu<sub>3</sub>O<sub>7</sub> isolation layer used in our devices.</p></div>","PeriodicalId":100110,"journal":{"name":"Applied Superconductivity","volume":"6 10","pages":"Pages 663-667"},"PeriodicalIF":0.0000,"publicationDate":"1999-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0964-1807(99)00026-5","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0964180799000265","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
For many SQUID applications robust, compact magnetometers are required with low flux noise and high effective area at 77 K. Low flux noise is achieved by using a low inductance SQUID. A low inductance SQUID will also have a high transfer function, allowing simplified direct readout schemes to be used. For maximum field sensitivity the SQUID needs to be coupled to a pickup loop of large area and therefore large inductance. We have modelled, designed and fabricated a novel HTS magnetometer consisting of a low inductance (<16 pH) dc SQUID coupled to a 28 nH pickup loop flux transformer fabricated on the same 1 cm2 substrate. Efficient coupling was achieved by using a flip-chipped intermediate flux transformer. This configuration produces a magnetometer with a high sensitivity per unit area. The magnetometers incorporate PrBa2Cu3O7 isolation layers and two 2 μm diameter CAM variant junctions. Thick YBa2Cu3O7 layers were used to improve coupling and decrease the demagnetisation factor wherever possible. Our device had a transfer function of 913μV/Φ0 which allows direct readout without any matching or additional positive feedback arrangements. The measured effective area at 77 K was 0.58 mm2 (3.6 nT/Φ0). The magnetometer white noise was 18 fT/ and at 1 Hz was 380 fT/. This was reduced at 1 Hz to 120 fT/ using bias reversal. The measured white noise was higher than the design value and is largely due to Johnson noise from the PrBa2Cu3O7 isolation layer used in our devices.