Magnetic properties of YBCO/LCMO superlattices with and without STO interlayers

dc.contributorUniversidade Estadual Paulista (UNESP)
dc.creatorYonamine, Anne Hitomi
dc.creatorFedossev, Sergey A.
dc.creatorSantos, Dayse Iara dos
dc.creatorPan, Alexey V.
dc.date2016-03-02T13:03:31Z
dc.date2016-10-25T21:33:03Z
dc.date2016-03-02T13:03:31Z
dc.date2016-10-25T21:33:03Z
dc.date2014
dc.date.accessioned2017-04-06T10:05:45Z
dc.date.available2017-04-06T10:05:45Z
dc.identifierAdvanced Materials Research, v. 975, p. 101-105, 2014.
dc.identifier1662-8985
dc.identifierhttp://hdl.handle.net/11449/135605
dc.identifierhttp://acervodigital.unesp.br/handle/11449/135605
dc.identifier10.4028/www.scientific.net/AMR.975.101
dc.identifier8506867595279427
dc.identifierhttp://dx.doi.org/10.4028/www.scientific.net/AMR.975.101
dc.identifier.urihttp://repositorioslatinoamericanos.uchile.cl/handle/2250/946111
dc.descriptionSuperlattices formed of two antagonic characteristics have been broadly studied in literature mainly in order to clarify the effects of proximity and interface interactions. Here, we present a study of superlattice introducing an insulator between each superconducting and ferromagnetic layer. The electrical insulator STO, YBCO and LCMO layer are deposited by PLD method. The samples with STO show more intergrowth surface morphology, which favors the application providing better contacts between the grains. The magnetic measurements indicated higher Tc values and high anisotropy for SLs with STO, which is dependent on the relative thickness of LCMO and YBCO.
dc.languageeng
dc.relationAdvanced Materials Research
dc.rightsinfo:eu-repo/semantics/closedAccess
dc.subjectSuperconducting devices
dc.subjectSuperlattices
dc.subjectSuperredes YBCO/LCMO
dc.titleMagnetic properties of YBCO/LCMO superlattices with and without STO interlayers
dc.typeOtro


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