000894054 001__ 894054
000894054 005__ 20250129094300.0
000894054 0247_ $$2Handle$$a2128/28186
000894054 037__ $$aFZJ-2021-03008
000894054 041__ $$aEnglish
000894054 1001_ $$0P:(DE-Juel1)172029$$aStellhorn, A.$$b0$$ufzj
000894054 1112_ $$a725. WE-Heraeus-Seminar: Magnetic Small Angle Neutron Scattering – from Nanoscale Magnetism to Long‐Range Magnetic Structures$$conline event$$d2021-05-31 - 2021-06-03$$wonline event
000894054 245__ $$aInterplay of proximity effects in Superconductor/Ferromagnet heterostructures
000894054 260__ $$c2021
000894054 3367_ $$0PUB:(DE-HGF)1$$2PUB:(DE-HGF)$$aAbstract$$babstract$$mabstract$$s1626258717_17130
000894054 3367_ $$033$$2EndNote$$aConference Paper
000894054 3367_ $$2BibTeX$$aINPROCEEDINGS
000894054 3367_ $$2DRIVER$$aconferenceObject
000894054 3367_ $$2DataCite$$aOutput Types/Conference Abstract
000894054 3367_ $$2ORCID$$aOTHER
000894054 520__ $$aProximity effects in superconductor/ferromagnet thin film heterostructures are ahighly topical issue due to their potential application in superconducting spin valvesor fluxonic devices [1, 2]. Physical properties can be controlled by an appliedmagnetic field and emerge for example as stray-field generated domainsuperconductivityor spin-triplet correlations. Our goal is to investigate their interplayand tunability by an external magnetic field. We use a heterostructure system ofNb/FePd with varying strength of magnetocrystalline anisotropy and a lateral domainstructure, grown by molecular beam epitaxy.On the one hand, macroscopic magnetoelectric transport measurements reveal aconfined superconducting state due to the stray fields of L10-ordered FePd. On theother hand, direct proximity effects at the Nb/FePd interface with a non-collinearmagnetization presumably lead to the generation of spin-triplet Cooper paircomponents with long penetration depth within the ferromagnetic layer [3]. PolarizedGrazing-Incidence Small-Angle Neutron Scattering (GISANS) probe exchangemechanisms on the microscopic scale and reveal a change in the ferromagneticdomain pattern by an onset of domain-wall-superconductivity. This mechanismcannot be revealed by macroscopic magnetization measurements, which makesGISANS the method of choice for detecting inverse superconducting proximityeffects.
000894054 536__ $$0G:(DE-HGF)POF4-632$$a632 - Materials – Quantum, Complex and Functional Materials (POF4-632)$$cPOF4-632$$fPOF IV$$x0
000894054 536__ $$0G:(DE-HGF)POF4-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (FZJ) (POF4-6G4)$$cPOF4-6G4$$fPOF IV$$x1
000894054 7001_ $$0P:(DE-Juel1)130754$$aKentzinger, Emmanuel$$b1$$ufzj
000894054 7001_ $$0P:(DE-Juel1)172634$$aSarkar, Anirban$$b2
000894054 7001_ $$0P:(DE-Juel1)130893$$aPipich, Vitaliy$$b3$$ufzj
000894054 7001_ $$0P:(DE-HGF)0$$aKrycka, Kathryn$$b4
000894054 7001_ $$0P:(DE-Juel1)169442$$aSchöffmann, Patrick$$b5$$ufzj
000894054 7001_ $$0P:(DE-Juel1)173818$$aBhatnagar, Tanvi$$b6$$ufzj
000894054 7001_ $$0P:(DE-Juel1)130572$$aBrückel, Thomas$$b7$$ufzj
000894054 8564_ $$uhttps://juser.fz-juelich.de/record/894054/files/abstract%20stellhorn.pdf$$yOpenAccess
000894054 909CO $$ooai:juser.fz-juelich.de:894054$$pVDB:MLZ$$pdriver$$pVDB$$popen_access$$popenaire
000894054 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)172029$$aForschungszentrum Jülich$$b0$$kFZJ
000894054 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130754$$aForschungszentrum Jülich$$b1$$kFZJ
000894054 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130893$$aForschungszentrum Jülich$$b3$$kFZJ
000894054 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)169442$$aForschungszentrum Jülich$$b5$$kFZJ
000894054 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)173818$$aForschungszentrum Jülich$$b6$$kFZJ
000894054 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130572$$aForschungszentrum Jülich$$b7$$kFZJ
000894054 9131_ $$0G:(DE-HGF)POF4-632$$1G:(DE-HGF)POF4-630$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lFrom Matter to Materials and Life$$vMaterials – Quantum, Complex and Functional Materials$$x0
000894054 9131_ $$0G:(DE-HGF)POF4-6G4$$1G:(DE-HGF)POF4-6G0$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lGroßgeräte: Materie$$vJülich Centre for Neutron Research (JCNS) (FZJ)$$x1
000894054 9141_ $$y2021
000894054 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000894054 9201_ $$0I:(DE-Juel1)JCNS-2-20110106$$kJCNS-2$$lStreumethoden$$x0
000894054 9201_ $$0I:(DE-Juel1)PGI-4-20110106$$kPGI-4$$lStreumethoden$$x1
000894054 9201_ $$0I:(DE-82)080009_20140620$$kJARA-FIT$$lJARA-FIT$$x2
000894054 9201_ $$0I:(DE-Juel1)JCNS-FRM-II-20110218$$kJCNS-FRM-II$$lJCNS-FRM-II$$x3
000894054 9801_ $$aFullTexts
000894054 980__ $$aabstract
000894054 980__ $$aVDB
000894054 980__ $$aUNRESTRICTED
000894054 980__ $$aI:(DE-Juel1)JCNS-2-20110106
000894054 980__ $$aI:(DE-Juel1)PGI-4-20110106
000894054 980__ $$aI:(DE-82)080009_20140620
000894054 980__ $$aI:(DE-Juel1)JCNS-FRM-II-20110218
000894054 981__ $$aI:(DE-Juel1)JCNS-2-20110106