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dc.contributor.authorShaltiel, D.en_US
dc.contributor.authorvon Nidda, H-A Krugen_US
dc.contributor.authorRosenstein, B.en_US
dc.contributor.authorShapiro, B. Yaen_US
dc.contributor.authorGolosovsky, M.en_US
dc.contributor.authorShapiro, I.en_US
dc.contributor.authorLoidl, A.en_US
dc.contributor.authorBogoslavsky, B.en_US
dc.contributor.authorFujii, T.en_US
dc.contributor.authorWatanabe, T.en_US
dc.contributor.authorTamegai, T.en_US
dc.date.accessioned2014-12-08T15:06:40Z-
dc.date.available2014-12-08T15:06:40Z-
dc.date.issued2010-07-01en_US
dc.identifier.issn0953-2048en_US
dc.identifier.urihttp://dx.doi.org/10.1088/0953-2048/23/7/075001en_US
dc.identifier.urihttp://hdl.handle.net/11536/5214-
dc.description.abstractA memory effect in the Josephson vortex system created by a magnetic field in the highly anisotropic superconductors Bi2212 and Bi2223 is demonstrated using microwave power absorption. This surprising effect appears despite a very low viscosity of Josephson vortices compared to Abrikosov vortices. The superconductor is field-cooled in a DC magnetic field H(m) oriented parallel to the CuO planes through the critical temperature T(c) down to 4 K, with subsequent reduction of the field to zero and again above H(m). A large microwave power absorption signal is observed at a magnetic field just above the cooling field, clearly indicating a memory effect. The dependence of the signal on a deviation of the magnetic field from H(m) is the same for a wide range of H(m) from 1500 to 17 000 G.en_US
dc.language.isoen_USen_US
dc.titleField cooling memory effect in Bi2212 and Bi2223 single crystalsen_US
dc.typeArticleen_US
dc.identifier.doi10.1088/0953-2048/23/7/075001en_US
dc.identifier.journalSUPERCONDUCTOR SCIENCE & TECHNOLOGYen_US
dc.citation.volume23en_US
dc.citation.issue7en_US
dc.citation.epageen_US
dc.contributor.department電子物理學系zh_TW
dc.contributor.departmentDepartment of Electrophysicsen_US
dc.identifier.wosnumberWOS:000279873400003-
dc.citation.woscount2-
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