Magnetic Relaxation in a Y 0.5Lu0.5Ba2Cu3O y Superconductor at Various Magnetization Levels

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The evolution of the rate of flux creep along the major hysteresis envelopes in a Y0.5Lu0.5Ba2Ca3Oy sample synthesized by a modified melt powder melt growth (MPMG) method at 25 K has been investigated. Magnetic relaxation rates depend strongly on the prior magnetic history. Calculations based on the critical state model can reproduce quite well the experimental data for magnetization when we have chosen the field exponent n = 0.3 in critical current density, Jc(Ha) = Jc0/(Ha−IM)n, where IM = Ha when 0 < H < Hc1 and (Formula presented.) when Ha ≥ Hc1. Using the field-cooled magnetization MFC data as well as the comparison of experimental and calculated M–H hysteresis loop, we estimated Hc1 = 500 Oe, p = 0, and the penetration field H∗ = 20 kOe. The apparent pinning energy was estimated as 62 meV for the remanent magnetization upon an excursion of 40 kOe.

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AlanDeğerDil
dc.contributor.authorÇelebi, S.
dc.contributor.authorOzturk, A.
dc.contributor.authorUysal, E.
dc.contributor.authorKutuk, S.
dc.contributor.authorDuzgun, I.
dc.date.accessioned2026-10-22T10:19:38.812036845Z
dc.date.available2026-10-22T10:19:38.812036845Z
dc.date.issued2015
dc.description.abstractThe evolution of the rate of flux creep along the major hysteresis envelopes in a Y0.5Lu0.5Ba2Ca3Oy sample synthesized by a modified melt powder melt growth (MPMG) method at 25 K has been investigated. Magnetic relaxation rates depend strongly on the prior magnetic history. Calculations based on the critical state model can reproduce quite well the experimental data for magnetization when we have chosen the field exponent n = 0.3 in critical current density, Jc(Ha) = Jc0/(Ha−IM)n, where IM = Ha when 0 < H < Hc1 and (Formula presented.) when Ha ≥ Hc1. Using the field-cooled magnetization MFC data as well as the comparison of experimental and calculated M–H hysteresis loop, we estimated Hc1 = 500 Oe, p = 0, and the penetration field H∗ = 20 kOe. The apparent pinning energy was estimated as 62 meV for the remanent magnetization upon an excursion of 40 kOe.
dc.identifier.doi10.1007/s10948-014-2851-2
dc.identifier.eissn1557-1947
dc.identifier.endpage39
dc.identifier.issn1557-1939
dc.identifier.issue1
dc.identifier.scopus2-s2.0-84925533014
dc.identifier.startpage33
dc.identifier.urihttps://rdlopen.rawdatalibrary.net/r/gumushane/12070
dc.identifier.volume28
dc.identifier.wosWOS:000349350500006
dc.language.isoen
dc.publisherSpringer Science and Business Media, LLC
dc.relation.ispartofJournal of Superconductivity and Novel Magnetism
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.subjectCritical current density
dc.subjectCritical state model
dc.subjectLu doping
dc.subjectMagnetic relaxation rate
dc.subjectMagnetization
dc.subjectYBCO superconductor
dc.subject.classificationPhysics, Applied
dc.subject.classificationPhysics, Condensed Matter
dc.subject.classificationPhysics
dc.subject.otherBarium compounds
dc.subject.otherCalcium compounds
dc.subject.otherCritical current density (superconductivity)
dc.subject.otherHysteresis
dc.subject.otherMagnetic materials
dc.subject.otherMagnetic relaxation
dc.subject.otherSuperconducting materials
dc.subject.otherYttrium barium copper oxides
dc.subject.otherCritical state models
dc.subject.otherField-cooled magnetizations
dc.subject.otherFlux creep
dc.subject.otherMagnetic history
dc.subject.otherMelt growth
dc.subject.otherPinning energy
dc.subject.otherRemanent magnetization
dc.subject.otherYBCO superconductor
dc.subject.otherMagnetization
dc.titleMagnetic Relaxation in a Y 0.5Lu0.5Ba2Cu3O y Superconductor at Various Magnetization Levels
dc.typeArticle
rdl.citation.openalex0
rdl.citation.scopus0
rdl.citation.wos0
rdl.oa.statusclosed
rdl.scopus.quartileQ3
rdl.source.indexSCOPUS
rdl.source.indexWOS
rdl.wos.indexScience Citation Index Expanded (SCI-EXPANDED)