000824626 001__ 824626 000824626 005__ 20210129225105.0 000824626 0247_ $$2doi$$a10.1039/C6NR01869F 000824626 0247_ $$2ISSN$$a2040-3364 000824626 0247_ $$2ISSN$$a2040-3372 000824626 0247_ $$2WOS$$aWOS:000376047200032 000824626 037__ $$aFZJ-2016-07189 000824626 082__ $$a600 000824626 1001_ $$0P:(DE-HGF)0$$aPrajapat, C. L.$$b0 000824626 245__ $$aSuperconductivity-induced magnetization depletion in a ferromagnet through an insulator in a ferromagnet–insulator–superconductor hybrid oxide heterostructure 000824626 260__ $$aCambridge$$bRSC Publ.$$c2016 000824626 3367_ $$2DRIVER$$aarticle 000824626 3367_ $$2DataCite$$aOutput Types/Journal article 000824626 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1484727763_22338 000824626 3367_ $$2BibTeX$$aARTICLE 000824626 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000824626 3367_ $$00$$2EndNote$$aJournal Article 000824626 520__ $$aCoupling between superconducting and ferromagnetic states in hybrid oxide heterostructures is presently a topic of intense research. Such a coupling is due to the leakage of the Cooper pairs into the ferromagnet. However, tunneling of the Cooper pairs though an insulator was never considered plausible. Using depth sensitive polarized neutron reflectivity we demonstrate the coupling between superconductor and magnetic layers in epitaxial La2/3Ca1/3MnO3 (LCMO)/SrTiO3/YBa2Cu3O7−δ (YBCO) hybrid heterostructures, with SrTiO3 as an intervening oxide insulator layer between the ferromagnet and the superconductor. Measurements above and below the superconducting transition temperature (TSC) of YBCO demonstrate a large modulation of magnetization in the ferromagnetic layer below the TSC of YBCO in these heterostructures. This work highlights a unique tunneling phenomenon between the epitaxial layers of an oxide superconductor (YBCO) and a magnetic layer (LCMO) through an insulating layer. Our work would inspire further investigations on the fundamental aspect of a long range order of the triplet spin-pairing in hybrid structures 000824626 536__ $$0G:(DE-HGF)POF3-6G15$$a6G15 - FRM II / MLZ (POF3-6G15)$$cPOF3-6G15$$fPOF III$$x0 000824626 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x1 000824626 588__ $$aDataset connected to CrossRef 000824626 65027 $$0V:(DE-MLZ)SciArea-170$$2V:(DE-HGF)$$aMagnetism$$x0 000824626 65017 $$0V:(DE-MLZ)GC-1604-2016$$2V:(DE-HGF)$$aMagnetic Materials$$x0 000824626 693__ $$0EXP:(DE-MLZ)MARIA-20140101$$1EXP:(DE-MLZ)FRMII-20140101$$5EXP:(DE-MLZ)MARIA-20140101$$6EXP:(DE-MLZ)NL5N-20140101$$aForschungs-Neutronenquelle Heinz Maier-Leibnitz $$eMARIA: Magnetic reflectometer with high incident angle$$fNL5N$$x0 000824626 7001_ $$0P:(DE-HGF)0$$aSingh, Surendra$$b1$$eCorresponding author 000824626 7001_ $$0P:(DE-HGF)0$$aPaul, Amitesh$$b2$$eCorresponding author 000824626 7001_ $$0P:(DE-HGF)0$$aBhattacharya, D.$$b3 000824626 7001_ $$0P:(DE-HGF)0$$aSingh, M. 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