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Decomposing the Bragg glass and the peak effect in a Type-II superconductor
Adding impurities or defects destroys crystalline order. Occasionally, however, extraordinary behaviour emerges that cannot be explained by perturbing the ordered state. One example is the Kondo effect, where magnetic impurities in metals drastically alter the temperature dependence of resistivity....
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Published in: | Nature communications 2018-03, Vol.9 (1), p.901-12, Article 901 |
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description | Adding impurities or defects destroys crystalline order. Occasionally, however, extraordinary behaviour emerges that cannot be explained by perturbing the ordered state. One example is the Kondo effect, where magnetic impurities in metals drastically alter the temperature dependence of resistivity. In Type-II superconductors, disorder generally works to pin vortices, giving zero resistivity below a critical current
j
c
. However, peaks have been observed in the temperature and field dependences of
j
c
. This peak effect is difficult to explain in terms of an ordered Abrikosov vortex lattice. Here we test the widespread paradigm that an order-disorder transition of the vortex ensemble drives the peak effect. Using neutron scattering to probe the vortex order in superconducting vanadium, we uncover an order-disorder transition from a quasi-long-range-ordered phase to a vortex glass. The peak effect, however, is found to lie at higher fields and temperatures, in a region where thermal fluctuations of individual vortices become significant.
The disordering of the vortex lattice in a type-II superconductor is widely perceived to underpin unusual peaks in the temperature and field dependence of critical current. By contrast, here Toft-Petersen et al. find an order-disorder transition in a superconducting vanadium sample that is unconnected with peaks observed in critical current. |
doi_str_mv | 10.1038/s41467-018-03267-z |
format | article |
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j
c
. However, peaks have been observed in the temperature and field dependences of
j
c
. This peak effect is difficult to explain in terms of an ordered Abrikosov vortex lattice. Here we test the widespread paradigm that an order-disorder transition of the vortex ensemble drives the peak effect. Using neutron scattering to probe the vortex order in superconducting vanadium, we uncover an order-disorder transition from a quasi-long-range-ordered phase to a vortex glass. The peak effect, however, is found to lie at higher fields and temperatures, in a region where thermal fluctuations of individual vortices become significant.
The disordering of the vortex lattice in a type-II superconductor is widely perceived to underpin unusual peaks in the temperature and field dependence of critical current. By contrast, here Toft-Petersen et al. find an order-disorder transition in a superconducting vanadium sample that is unconnected with peaks observed in critical current.</description><identifier>ISSN: 2041-1723</identifier><identifier>EISSN: 2041-1723</identifier><identifier>DOI: 10.1038/s41467-018-03267-z</identifier><identifier>PMID: 29500437</identifier><language>eng</language><publisher>London: Nature Publishing Group UK</publisher><subject>639/166/987 ; 639/301/119/1003 ; 639/766/119/1002 ; Critical current (superconductivity) ; Crystal defects ; Electrical resistivity ; Electrons ; Heavy metals ; Humanities and Social Sciences ; Impurities ; Kondo effect ; multidisciplinary ; Neutron scattering ; Neutrons ; Order-disorder transformations ; Phase transitions ; Science ; Science (multidisciplinary) ; Superconductivity ; Temperature dependence ; Vanadium ; Variation ; Vortices</subject><ispartof>Nature communications, 2018-03, Vol.9 (1), p.901-12, Article 901</ispartof><rights>The Author(s) 2018</rights><rights>2018. This work is published under http://creativecommons.org/licenses/by/4.0/ (the “License”). Notwithstanding the ProQuest Terms and Conditions, you may use this content in accordance with the terms of the License.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c606t-ff6eb75e4d72e6756199675968ab7696ffca64578b3fc107f9bb7d9ad9bd93073</citedby><cites>FETCH-LOGICAL-c606t-ff6eb75e4d72e6756199675968ab7696ffca64578b3fc107f9bb7d9ad9bd93073</cites><orcidid>0000-0001-7638-3675 ; 0000-0002-1556-3565 ; 0000-0002-3286-1118</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.proquest.com/docview/2009877787/fulltextPDF?pq-origsite=primo$$EPDF$$P50$$Gproquest$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.proquest.com/docview/2009877787?pq-origsite=primo$$EHTML$$P50$$Gproquest$$Hfree_for_read</linktohtml><link.rule.ids>230,314,727,780,784,885,25753,27924,27925,37012,37013,44590,53791,53793,75126</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/29500437$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Toft-Petersen, Rasmus</creatorcontrib><creatorcontrib>Abrahamsen, Asger B.</creatorcontrib><creatorcontrib>Balog, Sandor</creatorcontrib><creatorcontrib>Porcar, Lionel</creatorcontrib><creatorcontrib>Laver, Mark</creatorcontrib><title>Decomposing the Bragg glass and the peak effect in a Type-II superconductor</title><title>Nature communications</title><addtitle>Nat Commun</addtitle><addtitle>Nat Commun</addtitle><description>Adding impurities or defects destroys crystalline order. Occasionally, however, extraordinary behaviour emerges that cannot be explained by perturbing the ordered state. One example is the Kondo effect, where magnetic impurities in metals drastically alter the temperature dependence of resistivity. In Type-II superconductors, disorder generally works to pin vortices, giving zero resistivity below a critical current
j
c
. However, peaks have been observed in the temperature and field dependences of
j
c
. This peak effect is difficult to explain in terms of an ordered Abrikosov vortex lattice. Here we test the widespread paradigm that an order-disorder transition of the vortex ensemble drives the peak effect. Using neutron scattering to probe the vortex order in superconducting vanadium, we uncover an order-disorder transition from a quasi-long-range-ordered phase to a vortex glass. The peak effect, however, is found to lie at higher fields and temperatures, in a region where thermal fluctuations of individual vortices become significant.
The disordering of the vortex lattice in a type-II superconductor is widely perceived to underpin unusual peaks in the temperature and field dependence of critical current. 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Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Toft-Petersen, Rasmus</au><au>Abrahamsen, Asger B.</au><au>Balog, Sandor</au><au>Porcar, Lionel</au><au>Laver, Mark</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Decomposing the Bragg glass and the peak effect in a Type-II superconductor</atitle><jtitle>Nature communications</jtitle><stitle>Nat Commun</stitle><addtitle>Nat Commun</addtitle><date>2018-03-02</date><risdate>2018</risdate><volume>9</volume><issue>1</issue><spage>901</spage><epage>12</epage><pages>901-12</pages><artnum>901</artnum><issn>2041-1723</issn><eissn>2041-1723</eissn><abstract>Adding impurities or defects destroys crystalline order. Occasionally, however, extraordinary behaviour emerges that cannot be explained by perturbing the ordered state. One example is the Kondo effect, where magnetic impurities in metals drastically alter the temperature dependence of resistivity. In Type-II superconductors, disorder generally works to pin vortices, giving zero resistivity below a critical current
j
c
. However, peaks have been observed in the temperature and field dependences of
j
c
. This peak effect is difficult to explain in terms of an ordered Abrikosov vortex lattice. Here we test the widespread paradigm that an order-disorder transition of the vortex ensemble drives the peak effect. Using neutron scattering to probe the vortex order in superconducting vanadium, we uncover an order-disorder transition from a quasi-long-range-ordered phase to a vortex glass. The peak effect, however, is found to lie at higher fields and temperatures, in a region where thermal fluctuations of individual vortices become significant.
The disordering of the vortex lattice in a type-II superconductor is widely perceived to underpin unusual peaks in the temperature and field dependence of critical current. By contrast, here Toft-Petersen et al. find an order-disorder transition in a superconducting vanadium sample that is unconnected with peaks observed in critical current.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>29500437</pmid><doi>10.1038/s41467-018-03267-z</doi><tpages>12</tpages><orcidid>https://orcid.org/0000-0001-7638-3675</orcidid><orcidid>https://orcid.org/0000-0002-1556-3565</orcidid><orcidid>https://orcid.org/0000-0002-3286-1118</orcidid><oa>free_for_read</oa></addata></record> |
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subjects | 639/166/987 639/301/119/1003 639/766/119/1002 Critical current (superconductivity) Crystal defects Electrical resistivity Electrons Heavy metals Humanities and Social Sciences Impurities Kondo effect multidisciplinary Neutron scattering Neutrons Order-disorder transformations Phase transitions Science Science (multidisciplinary) Superconductivity Temperature dependence Vanadium Variation Vortices |
title | Decomposing the Bragg glass and the peak effect in a Type-II superconductor |
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