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Pulsed laser deposition of novel HTS multilayers for passive and active device applications
Multilayered structures have been fabricated from binary combinations of the high-T/sub c/ superconductor YBa/sub 2/Cu/sub 3/O/sub 7- delta / (YBCO) and the ferrite BaFe/sub 12/O/sub 19/ (BFO) or the ferroelectric Sr/sub 0.5/Ba/sub 0.5/TiO/sub 3/ (SBT). The combination of YBCO and BFO was found to d...
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Published in: | IEEE transactions on applied superconductivity 1993-03, Vol.3 (1), p.1528-1531 |
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container_title | IEEE transactions on applied superconductivity |
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creator | Chrisey, D.B. Horwitz, J.S. Pond, J.M. Carrol, K.R. Lubitz, P. Grabowski, K.S. Leuchtner, R.E. Carosella, C.A. Vittoria, C.V. |
description | Multilayered structures have been fabricated from binary combinations of the high-T/sub c/ superconductor YBa/sub 2/Cu/sub 3/O/sub 7- delta / (YBCO) and the ferrite BaFe/sub 12/O/sub 19/ (BFO) or the ferroelectric Sr/sub 0.5/Ba/sub 0.5/TiO/sub 3/ (SBT). The combination of YBCO and BFO was found to destroy the superconductivity of the YBCO layer. Vibrating sample magnetometer measurements of the BFO layer still indicated a large uniaxial anisotropy. The underlying YBCO layer of an SBT/YBCO bilayer still had high quality transport properties unaffected by the SBT layer (T/sub c/ approximately 91 K. J/sub c/(77 K) approximately 2*10/sup 6/ A/cm/sup 2/). A thin-film, normal metal/SBT transmission line, patterned in microstrip, demonstrated a wealth of temperature and electric field dependent dielectric information for the frequency range tested (f |
doi_str_mv | 10.1109/77.233376 |
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The combination of YBCO and BFO was found to destroy the superconductivity of the YBCO layer. Vibrating sample magnetometer measurements of the BFO layer still indicated a large uniaxial anisotropy. The underlying YBCO layer of an SBT/YBCO bilayer still had high quality transport properties unaffected by the SBT layer (T/sub c/ approximately 91 K. J/sub c/(77 K) approximately 2*10/sup 6/ A/cm/sup 2/). A thin-film, normal metal/SBT transmission line, patterned in microstrip, demonstrated a wealth of temperature and electric field dependent dielectric information for the frequency range tested (f<or=3 GHz). At 100 K, the dielectric constant for zero applied field was 250 for frequencies less than 30 MHz; it was approximately 120 for 1 GHz<or=f<or=3 GHz, and it varied continuously with frequency between these values. For temperatures between 300 K and 11 K, frequencies less than about 0.5 GHz, and applied fields up to 200 kV/cm, a nearly linear change in field-induced phase difference was produced in the transmission line. Above this frequency the field dependence changed sign and essentially disappeared at approximately 1 GHz.< ></description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/77.233376</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Applied sciences ; Electronics ; Exact sciences and technology ; Ferrites ; Ferroelectric materials ; Frequency ; High temperature superconductors ; Nonhomogeneous media ; Optical pulses ; Pulsed laser deposition ; Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices ; Strontium ; Superconducting devices ; Superconducting transmission lines ; Yttrium barium copper oxide</subject><ispartof>IEEE transactions on applied superconductivity, 1993-03, Vol.3 (1), p.1528-1531</ispartof><rights>1994 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c238t-57bd3b4300e51a5912650d3361810222f7245d436f4694649c74c92d7f840c003</citedby><cites>FETCH-LOGICAL-c238t-57bd3b4300e51a5912650d3361810222f7245d436f4694649c74c92d7f840c003</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/233376$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>309,310,314,777,781,786,787,23912,23913,25122,27906,27907,54778</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=4126083$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Chrisey, D.B.</creatorcontrib><creatorcontrib>Horwitz, J.S.</creatorcontrib><creatorcontrib>Pond, J.M.</creatorcontrib><creatorcontrib>Carrol, K.R.</creatorcontrib><creatorcontrib>Lubitz, P.</creatorcontrib><creatorcontrib>Grabowski, K.S.</creatorcontrib><creatorcontrib>Leuchtner, R.E.</creatorcontrib><creatorcontrib>Carosella, C.A.</creatorcontrib><creatorcontrib>Vittoria, C.V.</creatorcontrib><title>Pulsed laser deposition of novel HTS multilayers for passive and active device applications</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>Multilayered structures have been fabricated from binary combinations of the high-T/sub c/ superconductor YBa/sub 2/Cu/sub 3/O/sub 7- delta / (YBCO) and the ferrite BaFe/sub 12/O/sub 19/ (BFO) or the ferroelectric Sr/sub 0.5/Ba/sub 0.5/TiO/sub 3/ (SBT). The combination of YBCO and BFO was found to destroy the superconductivity of the YBCO layer. Vibrating sample magnetometer measurements of the BFO layer still indicated a large uniaxial anisotropy. The underlying YBCO layer of an SBT/YBCO bilayer still had high quality transport properties unaffected by the SBT layer (T/sub c/ approximately 91 K. J/sub c/(77 K) approximately 2*10/sup 6/ A/cm/sup 2/). A thin-film, normal metal/SBT transmission line, patterned in microstrip, demonstrated a wealth of temperature and electric field dependent dielectric information for the frequency range tested (f<or=3 GHz). At 100 K, the dielectric constant for zero applied field was 250 for frequencies less than 30 MHz; it was approximately 120 for 1 GHz<or=f<or=3 GHz, and it varied continuously with frequency between these values. For temperatures between 300 K and 11 K, frequencies less than about 0.5 GHz, and applied fields up to 200 kV/cm, a nearly linear change in field-induced phase difference was produced in the transmission line. Above this frequency the field dependence changed sign and essentially disappeared at approximately 1 GHz.< ></description><subject>Applied sciences</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>Ferrites</subject><subject>Ferroelectric materials</subject><subject>Frequency</subject><subject>High temperature superconductors</subject><subject>Nonhomogeneous media</subject><subject>Optical pulses</subject><subject>Pulsed laser deposition</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</subject><subject>Strontium</subject><subject>Superconducting devices</subject><subject>Superconducting transmission lines</subject><subject>Yttrium barium copper oxide</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1993</creationdate><recordtype>article</recordtype><recordid>eNo9kE1LAzEQhoMoWKsHr55yEMHD1nxn9yhFrVBQsJ48LGk-IJJu1mS30H9vSktP8zLzzMMwANxiNMMYNU9SzgilVIozMMGc1xXhmJ-XjDiuakLoJbjK-RchzGrGJ-DncwzZGhhUtgka28fsBx87GB3s4tYGuFh9wc0YBh_UzqYMXUywVzn7rYWqM1DpYR-N3XpdOn0fvFZ7Rb4GF04V-82xTsH368tqvqiWH2_v8-dlpQmth4rLtaFrRhGyHCveYCI4MpQKXGNECHGSMG4YFY6JhgnWaMl0Q4x0NUMaIToFDwdvn-LfaPPQbnzWNgTV2TjmlohiEZQX8PEA6hRzTta1ffIblXYtRu3-fa2U7eF9hb0_SlXWKrikOu3zaYGVK1FNC3Z3wLy19jQ9Ov4Bz8t1tw</recordid><startdate>19930301</startdate><enddate>19930301</enddate><creator>Chrisey, D.B.</creator><creator>Horwitz, J.S.</creator><creator>Pond, J.M.</creator><creator>Carrol, K.R.</creator><creator>Lubitz, P.</creator><creator>Grabowski, K.S.</creator><creator>Leuchtner, R.E.</creator><creator>Carosella, C.A.</creator><creator>Vittoria, C.V.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>19930301</creationdate><title>Pulsed laser deposition of novel HTS multilayers for passive and active device applications</title><author>Chrisey, D.B. ; Horwitz, J.S. ; Pond, J.M. ; Carrol, K.R. ; Lubitz, P. ; Grabowski, K.S. ; Leuchtner, R.E. ; Carosella, C.A. ; Vittoria, C.V.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c238t-57bd3b4300e51a5912650d3361810222f7245d436f4694649c74c92d7f840c003</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1993</creationdate><topic>Applied sciences</topic><topic>Electronics</topic><topic>Exact sciences and technology</topic><topic>Ferrites</topic><topic>Ferroelectric materials</topic><topic>Frequency</topic><topic>High temperature superconductors</topic><topic>Nonhomogeneous media</topic><topic>Optical pulses</topic><topic>Pulsed laser deposition</topic><topic>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</topic><topic>Strontium</topic><topic>Superconducting devices</topic><topic>Superconducting transmission lines</topic><topic>Yttrium barium copper oxide</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chrisey, D.B.</creatorcontrib><creatorcontrib>Horwitz, J.S.</creatorcontrib><creatorcontrib>Pond, J.M.</creatorcontrib><creatorcontrib>Carrol, K.R.</creatorcontrib><creatorcontrib>Lubitz, P.</creatorcontrib><creatorcontrib>Grabowski, K.S.</creatorcontrib><creatorcontrib>Leuchtner, R.E.</creatorcontrib><creatorcontrib>Carosella, C.A.</creatorcontrib><creatorcontrib>Vittoria, C.V.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE transactions on applied superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chrisey, D.B.</au><au>Horwitz, J.S.</au><au>Pond, J.M.</au><au>Carrol, K.R.</au><au>Lubitz, P.</au><au>Grabowski, K.S.</au><au>Leuchtner, R.E.</au><au>Carosella, C.A.</au><au>Vittoria, C.V.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Pulsed laser deposition of novel HTS multilayers for passive and active device applications</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>1993-03-01</date><risdate>1993</risdate><volume>3</volume><issue>1</issue><spage>1528</spage><epage>1531</epage><pages>1528-1531</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>Multilayered structures have been fabricated from binary combinations of the high-T/sub c/ superconductor YBa/sub 2/Cu/sub 3/O/sub 7- delta / (YBCO) and the ferrite BaFe/sub 12/O/sub 19/ (BFO) or the ferroelectric Sr/sub 0.5/Ba/sub 0.5/TiO/sub 3/ (SBT). The combination of YBCO and BFO was found to destroy the superconductivity of the YBCO layer. Vibrating sample magnetometer measurements of the BFO layer still indicated a large uniaxial anisotropy. The underlying YBCO layer of an SBT/YBCO bilayer still had high quality transport properties unaffected by the SBT layer (T/sub c/ approximately 91 K. J/sub c/(77 K) approximately 2*10/sup 6/ A/cm/sup 2/). A thin-film, normal metal/SBT transmission line, patterned in microstrip, demonstrated a wealth of temperature and electric field dependent dielectric information for the frequency range tested (f<or=3 GHz). At 100 K, the dielectric constant for zero applied field was 250 for frequencies less than 30 MHz; it was approximately 120 for 1 GHz<or=f<or=3 GHz, and it varied continuously with frequency between these values. For temperatures between 300 K and 11 K, frequencies less than about 0.5 GHz, and applied fields up to 200 kV/cm, a nearly linear change in field-induced phase difference was produced in the transmission line. Above this frequency the field dependence changed sign and essentially disappeared at approximately 1 GHz.< ></abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/77.233376</doi><tpages>4</tpages></addata></record> |
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subjects | Applied sciences Electronics Exact sciences and technology Ferrites Ferroelectric materials Frequency High temperature superconductors Nonhomogeneous media Optical pulses Pulsed laser deposition Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices Strontium Superconducting devices Superconducting transmission lines Yttrium barium copper oxide |
title | Pulsed laser deposition of novel HTS multilayers for passive and active device applications |
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