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Magnetization and relaxation in Hg-1223: bulk vs. surface irreversibility, anisotropy and the influence of Re-doping
Particle-size fractionization is used to separate bulk and surface hysteresis in pure and Re-doped Hg(15%)-1223. Re-doped samples have smaller surface barriers and higher bulk current densities than undoped Hg-1223. Neutron-irradiated samples exhibit practically no surface barrier effect. A `pinning...
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Published in: | Physica. C, Superconductivity Superconductivity, 1999-03, Vol.314 (1), p.81-92 |
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container_title | Physica. C, Superconductivity |
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creator | Krelaus, J. Reder, M. Hoffmann, J. Freyhardt, H.C. |
description | Particle-size fractionization is used to separate bulk and surface hysteresis in pure and Re-doped Hg(15%)-1223. Re-doped samples have smaller surface barriers and higher bulk current densities than undoped Hg-1223. Neutron-irradiated samples exhibit practically no surface barrier effect. A `pinning roughness' model is suggested to unify the observations. The fractionization technique is extended to relaxation of magnetically aligned Hg-1223. In wide temperature regions, both surface and bulk currents do relax. However, near the irreversibility temperature, bulk currents decay to zero, whereas surface relaxation continues. Relaxation is a complex interplay of bulk/surface effects, which subsequent investigations in this field must regard. From magnetization measurements on magnetically oriented samples, anisotropy parameters are estimated to
γ≈9±3 (Hg-1223) resp.
γ≈4.5±2 (Hg(15% Re)-1223). This is a very drastic effect of Re-doping on the superconducting properties of Hg-1223. |
doi_str_mv | 10.1016/S0921-4534(99)00149-5 |
format | article |
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γ≈9±3 (Hg-1223) resp.
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γ≈9±3 (Hg-1223) resp.
γ≈4.5±2 (Hg(15% Re)-1223). This is a very drastic effect of Re-doping on the superconducting properties of Hg-1223.</description><subject>Anisotropy</subject><subject>Hg-1223</subject><subject>Re-doping</subject><subject>Relaxation</subject><subject>Surface barrier</subject><issn>0921-4534</issn><issn>1873-2143</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1999</creationdate><recordtype>article</recordtype><recordid>eNqFkF1LwzAUhoMoOKc_QeiVKNiZpEmXeCMy1AkTwY_rkLanM9o1NUmH89ebbeKt5-Zw4HlfOA9CxwSPCCb5xTOWlKSMZ-xUyjOMCZMp30EDIsZZSgnLdtHgD9lHB96_4zhEkgEKD3reQjDfOhjbJrqtEgeN_tqepk2m85RQml0mRd98JEs_Snzval1CYpyDJThvCtOYsDqPYeNtcLZbbXrCW2TauumhjbStkydIK9uZdn6I9mrdeDj63UP0envzMpmms8e7-8n1LC0ZZiEtJNGUYqrpmJe5EFTUZV4JTvOc6HERF2WCZxgwI5hnUuc6E4TpQkjOAItsiE62vZ2znz34oBbGl9A0ugXbe0XHmPCoMIJ8C5bOeu-gVp0zC-1WimC1dqw2jtVaoJJSbRwrHnNX2xzEL5YGnPKlWb9bGQdlUJU1_zT8ALN3gns</recordid><startdate>19990301</startdate><enddate>19990301</enddate><creator>Krelaus, J.</creator><creator>Reder, M.</creator><creator>Hoffmann, J.</creator><creator>Freyhardt, H.C.</creator><general>Elsevier B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>19990301</creationdate><title>Magnetization and relaxation in Hg-1223: bulk vs. surface irreversibility, anisotropy and the influence of Re-doping</title><author>Krelaus, J. ; Reder, M. ; Hoffmann, J. ; Freyhardt, H.C.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c404t-b91a2202a275c68828fc6d852661a7b266248530e0410539a6a3814ab8954e083</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1999</creationdate><topic>Anisotropy</topic><topic>Hg-1223</topic><topic>Re-doping</topic><topic>Relaxation</topic><topic>Surface barrier</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Krelaus, J.</creatorcontrib><creatorcontrib>Reder, M.</creatorcontrib><creatorcontrib>Hoffmann, J.</creatorcontrib><creatorcontrib>Freyhardt, H.C.</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physica. C, Superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Krelaus, J.</au><au>Reder, M.</au><au>Hoffmann, J.</au><au>Freyhardt, H.C.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Magnetization and relaxation in Hg-1223: bulk vs. surface irreversibility, anisotropy and the influence of Re-doping</atitle><jtitle>Physica. C, Superconductivity</jtitle><date>1999-03-01</date><risdate>1999</risdate><volume>314</volume><issue>1</issue><spage>81</spage><epage>92</epage><pages>81-92</pages><issn>0921-4534</issn><eissn>1873-2143</eissn><abstract>Particle-size fractionization is used to separate bulk and surface hysteresis in pure and Re-doped Hg(15%)-1223. Re-doped samples have smaller surface barriers and higher bulk current densities than undoped Hg-1223. Neutron-irradiated samples exhibit practically no surface barrier effect. A `pinning roughness' model is suggested to unify the observations. The fractionization technique is extended to relaxation of magnetically aligned Hg-1223. In wide temperature regions, both surface and bulk currents do relax. However, near the irreversibility temperature, bulk currents decay to zero, whereas surface relaxation continues. Relaxation is a complex interplay of bulk/surface effects, which subsequent investigations in this field must regard. From magnetization measurements on magnetically oriented samples, anisotropy parameters are estimated to
γ≈9±3 (Hg-1223) resp.
γ≈4.5±2 (Hg(15% Re)-1223). This is a very drastic effect of Re-doping on the superconducting properties of Hg-1223.</abstract><pub>Elsevier B.V</pub><doi>10.1016/S0921-4534(99)00149-5</doi><tpages>12</tpages></addata></record> |
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subjects | Anisotropy Hg-1223 Re-doping Relaxation Surface barrier |
title | Magnetization and relaxation in Hg-1223: bulk vs. surface irreversibility, anisotropy and the influence of Re-doping |
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