Nicholas J. Exon, Mark N. Keene, Julian S. Satchell, Nigel G. Chew, Matthew J. Wooliscroft, Karan Lander, Richard G. Humphreys
{"title":"一种低噪声HTS SQUID磁强计,其片上拾取环路通过中间磁通变压器耦合","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":"{\"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}","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}
A low noise HTS SQUID magnetometer with an on-chip pickup loop coupled via an intermediate flux transformer
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.