Preparation and Properties of MgB2 Thin Films
The superconducting transition temperature of 140 nm ± 10 nm thin films on sapphire substrates, which were deposited by magnetron sputtering, was around 36 K. Using a magnetization technique, the film's critical current density was estimated as J C = 1.8 × 10 7 A/cm 2 at 10 K, J C = 8 × 10 6 A/...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2018-10, Vol.28 (7), p.1-7 |
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creator | Prikhna, Tatiana A. Eisterer, Michael Shaternik, Anton V. Shaternik, Volodymyr E. Seidel, Paul Sokolovsky, Vladimir Moshchil, Viktor E. Shapovalov, Andrii P. Romaka, Vitaliy V. Kovylaev, Valeriy V. Ponomaryov, Semyon S. |
description | The superconducting transition temperature of 140 nm ± 10 nm thin films on sapphire substrates, which were deposited by magnetron sputtering, was around 36 K. Using a magnetization technique, the film's critical current density was estimated as J C = 1.8 × 10 7 A/cm 2 at 10 K, J C = 8 × 10 6 A/m 2 at 20 K in a zero magnetic field B, and J C = 3 × 10 6 A/m 2 at 10 K and B = 5 T. The values of the upper critical magnetic field B c2 and the irreversibility field B irr estimated using the four-probe technique were B C2 (22 K) = 15 T when H||film surface, 11 T when H⊥film surface, and B irr (22 K) = 11 T when H||film surface. The X-ray study showed that the microstructure of the film contains only MgB 2 and MgO (in minority). The SEM and EPXMA study and quantitative Auger spectroscopy analysis revealed periodical variations of the film composition on the nanolevel and the presence of (mainly) two intercalated Mg-B-O-C phases of slightly different, especially in oxygen content, and thus with different conductivity and, possibly, with different T C . The characteristics of superconducting magnesium diboride films make them promising for application in electronic devices, e.g., as high-pass filters. |
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Using a magnetization technique, the film's critical current density was estimated as J C = 1.8 × 10 7 A/cm 2 at 10 K, J C = 8 × 10 6 A/m 2 at 20 K in a zero magnetic field B, and J C = 3 × 10 6 A/m 2 at 10 K and B = 5 T. The values of the upper critical magnetic field B c2 and the irreversibility field B irr estimated using the four-probe technique were B C2 (22 K) = 15 T when H||film surface, 11 T when H⊥film surface, and B irr (22 K) = 11 T when H||film surface. The X-ray study showed that the microstructure of the film contains only MgB 2 and MgO (in minority). The SEM and EPXMA study and quantitative Auger spectroscopy analysis revealed periodical variations of the film composition on the nanolevel and the presence of (mainly) two intercalated Mg-B-O-C phases of slightly different, especially in oxygen content, and thus with different conductivity and, possibly, with different T C . The characteristics of superconducting magnesium diboride films make them promising for application in electronic devices, e.g., as high-pass filters.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2018.2844357</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Auger spectroscopy ; Borides ; Critical current density ; Critical current density (superconductivity) ; Electronic devices ; field of irreversibility ; High pass filters ; High-temperature superconductors ; Magnesium ; Magnesium compounds ; Magnetic fields ; Magnetism ; Magnetron sputtering ; Oxygen content ; Sapphire ; Sputtering ; Substrates ; Superconducting filters ; Superconducting magnets ; Superconducting thin films ; Superconductivity ; Thin films ; Transition temperature ; upper critical field</subject><ispartof>IEEE transactions on applied superconductivity, 2018-10, Vol.28 (7), p.1-7</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2018</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/8373706$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,796,27924,27925,54758</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/8373706$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Prikhna, Tatiana A.</creatorcontrib><creatorcontrib>Eisterer, Michael</creatorcontrib><creatorcontrib>Shaternik, Anton V.</creatorcontrib><creatorcontrib>Shaternik, Volodymyr E.</creatorcontrib><creatorcontrib>Seidel, Paul</creatorcontrib><creatorcontrib>Sokolovsky, Vladimir</creatorcontrib><creatorcontrib>Moshchil, Viktor E.</creatorcontrib><creatorcontrib>Shapovalov, Andrii P.</creatorcontrib><creatorcontrib>Romaka, Vitaliy V.</creatorcontrib><creatorcontrib>Kovylaev, Valeriy V.</creatorcontrib><creatorcontrib>Ponomaryov, Semyon S.</creatorcontrib><title>Preparation and Properties of MgB2 Thin Films</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>The superconducting transition temperature of 140 nm ± 10 nm thin films on sapphire substrates, which were deposited by magnetron sputtering, was around 36 K. Using a magnetization technique, the film's critical current density was estimated as J C = 1.8 × 10 7 A/cm 2 at 10 K, J C = 8 × 10 6 A/m 2 at 20 K in a zero magnetic field B, and J C = 3 × 10 6 A/m 2 at 10 K and B = 5 T. The values of the upper critical magnetic field B c2 and the irreversibility field B irr estimated using the four-probe technique were B C2 (22 K) = 15 T when H||film surface, 11 T when H⊥film surface, and B irr (22 K) = 11 T when H||film surface. The X-ray study showed that the microstructure of the film contains only MgB 2 and MgO (in minority). The SEM and EPXMA study and quantitative Auger spectroscopy analysis revealed periodical variations of the film composition on the nanolevel and the presence of (mainly) two intercalated Mg-B-O-C phases of slightly different, especially in oxygen content, and thus with different conductivity and, possibly, with different T C . The characteristics of superconducting magnesium diboride films make them promising for application in electronic devices, e.g., as high-pass filters.</description><subject>Auger spectroscopy</subject><subject>Borides</subject><subject>Critical current density</subject><subject>Critical current density (superconductivity)</subject><subject>Electronic devices</subject><subject>field of irreversibility</subject><subject>High pass filters</subject><subject>High-temperature superconductors</subject><subject>Magnesium</subject><subject>Magnesium compounds</subject><subject>Magnetic fields</subject><subject>Magnetism</subject><subject>Magnetron sputtering</subject><subject>Oxygen content</subject><subject>Sapphire</subject><subject>Sputtering</subject><subject>Substrates</subject><subject>Superconducting filters</subject><subject>Superconducting magnets</subject><subject>Superconducting thin films</subject><subject>Superconductivity</subject><subject>Thin films</subject><subject>Transition temperature</subject><subject>upper critical field</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNotjUFLwzAYhoMoOKc_QLwUPLd-X5IvSY-zOBUmDqznEpdUM7a2Jt3Bf7_CPD3v4eF9GLtFKBChfKgXH1XBAU3BjZSC9BmbIZHJOSGdTxsIc8O5uGRXKW0BUBpJM5avox9stGPou8x2LlvHfvBxDD5lfZu9fT_yrP4JXbYMu326Zhet3SV_8885-1w-1dVLvnp_fq0WqzxwEGMuoVRSWOBKlEY6bkRrnLeloS_USpFtkSts9YY7C5KM0145rV2LtCnJGjFn96ffIfa_B5_GZtsfYjclG46okQRomKy7kxW8980Qw97Gv8YILTQocQSTYUuk</recordid><startdate>20181001</startdate><enddate>20181001</enddate><creator>Prikhna, Tatiana A.</creator><creator>Eisterer, Michael</creator><creator>Shaternik, Anton V.</creator><creator>Shaternik, Volodymyr E.</creator><creator>Seidel, Paul</creator><creator>Sokolovsky, Vladimir</creator><creator>Moshchil, Viktor E.</creator><creator>Shapovalov, Andrii P.</creator><creator>Romaka, Vitaliy V.</creator><creator>Kovylaev, Valeriy V.</creator><creator>Ponomaryov, Semyon S.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>20181001</creationdate><title>Preparation and Properties of MgB2 Thin Films</title><author>Prikhna, Tatiana A. ; Eisterer, Michael ; Shaternik, Anton V. ; Shaternik, Volodymyr E. ; Seidel, Paul ; Sokolovsky, Vladimir ; Moshchil, Viktor E. ; Shapovalov, Andrii P. ; Romaka, Vitaliy V. ; Kovylaev, Valeriy V. ; Ponomaryov, Semyon S.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-i203t-409643a0263984d283f8dea985b17665af1261f7c2da0458d7e6d77df15c95a83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Auger spectroscopy</topic><topic>Borides</topic><topic>Critical current density</topic><topic>Critical current density (superconductivity)</topic><topic>Electronic devices</topic><topic>field of irreversibility</topic><topic>High pass filters</topic><topic>High-temperature superconductors</topic><topic>Magnesium</topic><topic>Magnesium compounds</topic><topic>Magnetic fields</topic><topic>Magnetism</topic><topic>Magnetron sputtering</topic><topic>Oxygen content</topic><topic>Sapphire</topic><topic>Sputtering</topic><topic>Substrates</topic><topic>Superconducting filters</topic><topic>Superconducting magnets</topic><topic>Superconducting thin films</topic><topic>Superconductivity</topic><topic>Thin films</topic><topic>Transition temperature</topic><topic>upper critical field</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Prikhna, Tatiana A.</creatorcontrib><creatorcontrib>Eisterer, Michael</creatorcontrib><creatorcontrib>Shaternik, Anton V.</creatorcontrib><creatorcontrib>Shaternik, Volodymyr E.</creatorcontrib><creatorcontrib>Seidel, Paul</creatorcontrib><creatorcontrib>Sokolovsky, Vladimir</creatorcontrib><creatorcontrib>Moshchil, Viktor E.</creatorcontrib><creatorcontrib>Shapovalov, Andrii P.</creatorcontrib><creatorcontrib>Romaka, Vitaliy V.</creatorcontrib><creatorcontrib>Kovylaev, Valeriy V.</creatorcontrib><creatorcontrib>Ponomaryov, Semyon S.</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE Electronic Library (IEL)</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_linktorsrc</fulltext></delivery><addata><au>Prikhna, Tatiana A.</au><au>Eisterer, Michael</au><au>Shaternik, Anton V.</au><au>Shaternik, Volodymyr E.</au><au>Seidel, Paul</au><au>Sokolovsky, Vladimir</au><au>Moshchil, Viktor E.</au><au>Shapovalov, Andrii P.</au><au>Romaka, Vitaliy V.</au><au>Kovylaev, Valeriy V.</au><au>Ponomaryov, Semyon S.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Preparation and Properties of MgB2 Thin Films</atitle><jtitle>IEEE transactions on applied superconductivity</jtitle><stitle>TASC</stitle><date>2018-10-01</date><risdate>2018</risdate><volume>28</volume><issue>7</issue><spage>1</spage><epage>7</epage><pages>1-7</pages><issn>1051-8223</issn><eissn>1558-2515</eissn><coden>ITASE9</coden><abstract>The superconducting transition temperature of 140 nm ± 10 nm thin films on sapphire substrates, which were deposited by magnetron sputtering, was around 36 K. Using a magnetization technique, the film's critical current density was estimated as J C = 1.8 × 10 7 A/cm 2 at 10 K, J C = 8 × 10 6 A/m 2 at 20 K in a zero magnetic field B, and J C = 3 × 10 6 A/m 2 at 10 K and B = 5 T. The values of the upper critical magnetic field B c2 and the irreversibility field B irr estimated using the four-probe technique were B C2 (22 K) = 15 T when H||film surface, 11 T when H⊥film surface, and B irr (22 K) = 11 T when H||film surface. The X-ray study showed that the microstructure of the film contains only MgB 2 and MgO (in minority). The SEM and EPXMA study and quantitative Auger spectroscopy analysis revealed periodical variations of the film composition on the nanolevel and the presence of (mainly) two intercalated Mg-B-O-C phases of slightly different, especially in oxygen content, and thus with different conductivity and, possibly, with different T C . The characteristics of superconducting magnesium diboride films make them promising for application in electronic devices, e.g., as high-pass filters.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TASC.2018.2844357</doi><tpages>7</tpages></addata></record> |
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subjects | Auger spectroscopy Borides Critical current density Critical current density (superconductivity) Electronic devices field of irreversibility High pass filters High-temperature superconductors Magnesium Magnesium compounds Magnetic fields Magnetism Magnetron sputtering Oxygen content Sapphire Sputtering Substrates Superconducting filters Superconducting magnets Superconducting thin films Superconductivity Thin films Transition temperature upper critical field |
title | Preparation and Properties of MgB2 Thin Films |
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