Atomic layer by atomic layer growth of DyBaCuO superconducting thin films by molecular beam epitaxy
Superconducting thin films of DyBaCuO have been achieved by molecular beam epitaxy. The films are strongly oriented with the c axis perpendicular to the substrate, and currently reach R=0 between 70 and 80 K. Critical temperatures (R=0) up to 50 K were obtained on 150-Å-thick films deposited atomic...
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Veröffentlicht in: | Applied physics letters 1990-08, Vol.57 (8), p.819-821 |
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container_title | Applied physics letters |
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creator | Schuhl, A. Cabanel, R. Lequien, S. Ghyselen, B. Tyč, S. Creuzet, G. Siejka, J. |
description | Superconducting thin films of DyBaCuO have been achieved by molecular beam epitaxy. The films are strongly oriented with the c axis perpendicular to the substrate, and currently reach R=0 between 70 and 80 K. Critical temperatures (R=0) up to 50 K were obtained on 150-Å-thick films deposited atomic layer by atomic layer. These films present a flat surface as observed by high-energy electron diffraction. We show that in this process, a nominal 1:2:3 composition is not sufficient for the obtention of flat superconducting film. A good accuracy in the number of atoms deposited for each atomic layer is required. |
doi_str_mv | 10.1063/1.103430 |
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The films are strongly oriented with the c axis perpendicular to the substrate, and currently reach R=0 between 70 and 80 K. Critical temperatures (R=0) up to 50 K were obtained on 150-Å-thick films deposited atomic layer by atomic layer. These films present a flat surface as observed by high-energy electron diffraction. We show that in this process, a nominal 1:2:3 composition is not sufficient for the obtention of flat superconducting film. 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The films are strongly oriented with the c axis perpendicular to the substrate, and currently reach R=0 between 70 and 80 K. Critical temperatures (R=0) up to 50 K were obtained on 150-Å-thick films deposited atomic layer by atomic layer. These films present a flat surface as observed by high-energy electron diffraction. We show that in this process, a nominal 1:2:3 composition is not sufficient for the obtention of flat superconducting film. A good accuracy in the number of atoms deposited for each atomic layer is required.</description><subject>360202 - Ceramics, Cermets, & Refractories- Structure & Phase Studies</subject><subject>ALKALINE EARTH METAL COMPOUNDS</subject><subject>BARIUM COMPOUNDS</subject><subject>BARIUM OXIDES</subject><subject>CHALCOGENIDES</subject><subject>COHERENT SCATTERING</subject><subject>COPPER COMPOUNDS</subject><subject>COPPER OXIDES</subject><subject>CRYSTAL GROWTH</subject><subject>DIFFRACTION</subject><subject>DYSPROSIUM COMPOUNDS</subject><subject>DYSPROSIUM OXIDES</subject><subject>ELECTRON DIFFRACTION</subject><subject>EPITAXY</subject><subject>HIGH-TC SUPERCONDUCTORS</subject><subject>JOSEPHSON JUNCTIONS</subject><subject>JUNCTIONS</subject><subject>MATERIALS SCIENCE</subject><subject>MOLECULAR BEAM EPITAXY</subject><subject>OXIDES</subject><subject>OXYGEN COMPOUNDS</subject><subject>PHYSICAL PROPERTIES</subject><subject>RARE EARTH COMPOUNDS</subject><subject>SCATTERING</subject><subject>SUPERCONDUCTING FILMS</subject><subject>SUPERCONDUCTING JUNCTIONS</subject><subject>SUPERCONDUCTORS</subject><subject>THERMODYNAMIC PROPERTIES</subject><subject>TRANSITION ELEMENT COMPOUNDS</subject><subject>TRANSITION TEMPERATURE</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1990</creationdate><recordtype>article</recordtype><recordid>eNpNkEtLxDAcxIMouD7AjxA8iJdq0jSPHtf1CQt70XNIs__uRtqmJinab2-XevA0DPxmGAahK0ruKBHsnk7CCkaO0IISKTNGqTpGC0IIy0TJ6Sk6i_FzsjxnbIHsMvnWWdyYEQKuRmz--13w32mPfY0fxwezGjY4Dj0E67vtYJPrdjjtXYdr17TxEG59A3ZozNQEpsXQu2R-xgt0UpsmwuWfnqOP56f31Wu23ry8rZbrzDJOU7YVVVkSWYu8lEZamquKF5YpVfDKMllYWhoCNQGjGOQgJSfAVckUL_O8AmDn6Hru9TE5Ha1LYPfT1g5s0oIpKqWaoJsZ6oP_GiAm3bpooWlMB36IOudEyEKQCbydQRt8jAFq3QfXmjBqSvThak31fDX7Bc57b-k</recordid><startdate>19900820</startdate><enddate>19900820</enddate><creator>Schuhl, A.</creator><creator>Cabanel, R.</creator><creator>Lequien, S.</creator><creator>Ghyselen, B.</creator><creator>Tyč, S.</creator><creator>Creuzet, G.</creator><creator>Siejka, J.</creator><scope>AAYXX</scope><scope>CITATION</scope><scope>7SR</scope><scope>8FD</scope><scope>JG9</scope><scope>OTOTI</scope></search><sort><creationdate>19900820</creationdate><title>Atomic layer by atomic layer growth of DyBaCuO superconducting thin films by molecular beam epitaxy</title><author>Schuhl, A. ; Cabanel, R. ; Lequien, S. ; Ghyselen, B. ; Tyč, S. ; Creuzet, G. ; Siejka, J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c351t-d6b9907f6297a7c128b54c38845bc374c19a0ef0ea83e2e7750e589385922bee3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1990</creationdate><topic>360202 - Ceramics, Cermets, & Refractories- Structure & Phase Studies</topic><topic>ALKALINE EARTH METAL COMPOUNDS</topic><topic>BARIUM COMPOUNDS</topic><topic>BARIUM OXIDES</topic><topic>CHALCOGENIDES</topic><topic>COHERENT SCATTERING</topic><topic>COPPER COMPOUNDS</topic><topic>COPPER OXIDES</topic><topic>CRYSTAL GROWTH</topic><topic>DIFFRACTION</topic><topic>DYSPROSIUM COMPOUNDS</topic><topic>DYSPROSIUM OXIDES</topic><topic>ELECTRON DIFFRACTION</topic><topic>EPITAXY</topic><topic>HIGH-TC SUPERCONDUCTORS</topic><topic>JOSEPHSON JUNCTIONS</topic><topic>JUNCTIONS</topic><topic>MATERIALS SCIENCE</topic><topic>MOLECULAR BEAM EPITAXY</topic><topic>OXIDES</topic><topic>OXYGEN COMPOUNDS</topic><topic>PHYSICAL PROPERTIES</topic><topic>RARE EARTH COMPOUNDS</topic><topic>SCATTERING</topic><topic>SUPERCONDUCTING FILMS</topic><topic>SUPERCONDUCTING JUNCTIONS</topic><topic>SUPERCONDUCTORS</topic><topic>THERMODYNAMIC PROPERTIES</topic><topic>TRANSITION ELEMENT COMPOUNDS</topic><topic>TRANSITION TEMPERATURE</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Schuhl, A.</creatorcontrib><creatorcontrib>Cabanel, R.</creatorcontrib><creatorcontrib>Lequien, S.</creatorcontrib><creatorcontrib>Ghyselen, B.</creatorcontrib><creatorcontrib>Tyč, S.</creatorcontrib><creatorcontrib>Creuzet, G.</creatorcontrib><creatorcontrib>Siejka, J.</creatorcontrib><collection>CrossRef</collection><collection>Engineered Materials Abstracts</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>OSTI.GOV</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Schuhl, A.</au><au>Cabanel, R.</au><au>Lequien, S.</au><au>Ghyselen, B.</au><au>Tyč, S.</au><au>Creuzet, G.</au><au>Siejka, J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Atomic layer by atomic layer growth of DyBaCuO superconducting thin films by molecular beam epitaxy</atitle><jtitle>Applied physics letters</jtitle><date>1990-08-20</date><risdate>1990</risdate><volume>57</volume><issue>8</issue><spage>819</spage><epage>821</epage><pages>819-821</pages><issn>0003-6951</issn><eissn>1077-3118</eissn><abstract>Superconducting thin films of DyBaCuO have been achieved by molecular beam epitaxy. The films are strongly oriented with the c axis perpendicular to the substrate, and currently reach R=0 between 70 and 80 K. Critical temperatures (R=0) up to 50 K were obtained on 150-Å-thick films deposited atomic layer by atomic layer. These films present a flat surface as observed by high-energy electron diffraction. We show that in this process, a nominal 1:2:3 composition is not sufficient for the obtention of flat superconducting film. A good accuracy in the number of atoms deposited for each atomic layer is required.</abstract><cop>United States</cop><doi>10.1063/1.103430</doi><tpages>3</tpages></addata></record> |
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subjects | 360202 - Ceramics, Cermets, & Refractories- Structure & Phase Studies ALKALINE EARTH METAL COMPOUNDS BARIUM COMPOUNDS BARIUM OXIDES CHALCOGENIDES COHERENT SCATTERING COPPER COMPOUNDS COPPER OXIDES CRYSTAL GROWTH DIFFRACTION DYSPROSIUM COMPOUNDS DYSPROSIUM OXIDES ELECTRON DIFFRACTION EPITAXY HIGH-TC SUPERCONDUCTORS JOSEPHSON JUNCTIONS JUNCTIONS MATERIALS SCIENCE MOLECULAR BEAM EPITAXY OXIDES OXYGEN COMPOUNDS PHYSICAL PROPERTIES RARE EARTH COMPOUNDS SCATTERING SUPERCONDUCTING FILMS SUPERCONDUCTING JUNCTIONS SUPERCONDUCTORS THERMODYNAMIC PROPERTIES TRANSITION ELEMENT COMPOUNDS TRANSITION TEMPERATURE |
title | Atomic layer by atomic layer growth of DyBaCuO superconducting thin films by molecular beam epitaxy |
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