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Scaling of vortex lattice melting transition in single crystals of Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta )
The vortex lattice melting transition in single crystals Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) was studied by in-plane resistivity measurements in the Corbino geometry in magnetic fields tilted away from the c-axis. In strong contrast to YBa sub(2)Cu sub(3)O sub(7- delta ), the unusual non-e...
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Published in: | Physica. C, Superconductivity Superconductivity, 2001-08, Vol.357-360, p.450-453 |
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container_title | Physica. C, Superconductivity |
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creator | Mirkovic, J Savel'ev, S Sugahara, E Kadowaki, K |
description | The vortex lattice melting transition in single crystals Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) was studied by in-plane resistivity measurements in the Corbino geometry in magnetic fields tilted away from the c-axis. In strong contrast to YBa sub(2)Cu sub(3)O sub(7- delta ), the unusual non-elliptic melting transition line in the H super(c)-H super(ab) phase plane is observed. The H super(c)-H super(ab) melting curves measured in a wide temperature range, T < 88 K, collapse into the unique curve if the H super(c) and H super(ab) axes are rescaled by the functions H super(c)/(1-T/T sub(c)) super(1.3) and H super(ab)/(1-T super(2)/T super(2) sub(c)). This means that the effective anisotropy gamma super(eff) of the melting transition increases with temperature. At T approximately 88 K, the anisotropy gamma super(eff) exhibits maximum and tends to decrease close to T sub(c). copyright 2001 Elsevier Science B.V. All rights reserved. |
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In strong contrast to YBa sub(2)Cu sub(3)O sub(7- delta ), the unusual non-elliptic melting transition line in the H super(c)-H super(ab) phase plane is observed. The H super(c)-H super(ab) melting curves measured in a wide temperature range, T < 88 K, collapse into the unique curve if the H super(c) and H super(ab) axes are rescaled by the functions H super(c)/(1-T/T sub(c)) super(1.3) and H super(ab)/(1-T super(2)/T super(2) sub(c)). This means that the effective anisotropy gamma super(eff) of the melting transition increases with temperature. At T approximately 88 K, the anisotropy gamma super(eff) exhibits maximum and tends to decrease close to T sub(c). copyright 2001 Elsevier Science B.V. All rights reserved.</description><identifier>ISSN: 0921-4534</identifier><language>eng</language><ispartof>Physica. C, Superconductivity, 2001-08, Vol.357-360, p.450-453</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784</link.rule.ids></links><search><creatorcontrib>Mirkovic, J</creatorcontrib><creatorcontrib>Savel'ev, S</creatorcontrib><creatorcontrib>Sugahara, E</creatorcontrib><creatorcontrib>Kadowaki, K</creatorcontrib><title>Scaling of vortex lattice melting transition in single crystals of Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta )</title><title>Physica. C, Superconductivity</title><description>The vortex lattice melting transition in single crystals Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) was studied by in-plane resistivity measurements in the Corbino geometry in magnetic fields tilted away from the c-axis. In strong contrast to YBa sub(2)Cu sub(3)O sub(7- delta ), the unusual non-elliptic melting transition line in the H super(c)-H super(ab) phase plane is observed. The H super(c)-H super(ab) melting curves measured in a wide temperature range, T < 88 K, collapse into the unique curve if the H super(c) and H super(ab) axes are rescaled by the functions H super(c)/(1-T/T sub(c)) super(1.3) and H super(ab)/(1-T super(2)/T super(2) sub(c)). This means that the effective anisotropy gamma super(eff) of the melting transition increases with temperature. At T approximately 88 K, the anisotropy gamma super(eff) exhibits maximum and tends to decrease close to T sub(c). copyright 2001 Elsevier Science B.V. 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C, Superconductivity</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mirkovic, J</au><au>Savel'ev, S</au><au>Sugahara, E</au><au>Kadowaki, K</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Scaling of vortex lattice melting transition in single crystals of Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta )</atitle><jtitle>Physica. C, Superconductivity</jtitle><date>2001-08-01</date><risdate>2001</risdate><volume>357-360</volume><spage>450</spage><epage>453</epage><pages>450-453</pages><issn>0921-4534</issn><abstract>The vortex lattice melting transition in single crystals Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) was studied by in-plane resistivity measurements in the Corbino geometry in magnetic fields tilted away from the c-axis. In strong contrast to YBa sub(2)Cu sub(3)O sub(7- delta ), the unusual non-elliptic melting transition line in the H super(c)-H super(ab) phase plane is observed. The H super(c)-H super(ab) melting curves measured in a wide temperature range, T < 88 K, collapse into the unique curve if the H super(c) and H super(ab) axes are rescaled by the functions H super(c)/(1-T/T sub(c)) super(1.3) and H super(ab)/(1-T super(2)/T super(2) sub(c)). This means that the effective anisotropy gamma super(eff) of the melting transition increases with temperature. At T approximately 88 K, the anisotropy gamma super(eff) exhibits maximum and tends to decrease close to T sub(c). copyright 2001 Elsevier Science B.V. All rights reserved.</abstract></addata></record> |
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title | Scaling of vortex lattice melting transition in single crystals of Bi sub(2)Sr sub(2)CaCu sub(2)O sub(8+ delta ) |
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