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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
Main Authors: 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.
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cited_by cdi_FETCH-LOGICAL-c238t-57bd3b4300e51a5912650d3361810222f7245d436f4694649c74c92d7f840c003
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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&lt;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&lt;or=f&lt;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.&lt; &gt;</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. 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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&lt;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&lt;or=f&lt;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.&lt; &gt;</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 &amp; 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&lt;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&lt;or=f&lt;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.&lt; &gt;</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/77.233376</doi><tpages>4</tpages></addata></record>
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identifier ISSN: 1051-8223
ispartof IEEE transactions on applied superconductivity, 1993-03, Vol.3 (1), p.1528-1531
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1558-2515
language eng
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source IEEE Electronic Library (IEL) Journals
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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