Electric Polarity‐Dependent Modification of the Fe/BaTiO3 Interface
Source abstract
Abstract
The functionality and electronic properties of metal/ferroelectric systems rely heavily on the chemical and structural properties of the interface. The isotope sensitive technique of nuclear resonant scattering is used to selectively study the chemistry and magnetic state of the Fe/BaTiO3 interface. An electric polarity‐dependent modification of the metal/ferroelectric oxide interface has been systematically observed. The results show that the interface can be oxidized or reduced by inverting the polarity of the electric field applied across the interface above a threshold field value of ±400 kV m−1. Remarkably, the final interface state depends on the polarization history of the system. Based on these results, a model for the electric field induced ion transport at the Fe/BaTiO3 interface has been suggested. Such subtle structural changes at the interface deteriorate the magnetoelectric coupling. However, for certain applications where an oxide layer is required at metal/ferroelectric oxide interfaces, the electric fields can be used to control interdiffusion processes.
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Research context
OpenAlex topics: Multiferroics and related materials · Ferroelectric and Piezoelectric Materials · Geophysical Methods and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Instituut voor Kern‐en Stralingsfysica KU Leuven Celestijnenlaan 200D B‐3001 Leuven Belgium
European Synchrotron Radiation Facility (ESRF) 71 Avenue des Martyrs 38000 Grenoble France
Laboratorium voor Vaste‐Stoffysica en Magnetisme KU Leuven Celestijnenlaan 200D B‐3001 Leuven Belgium
Funding
Research Foundation Flanders (FWO) · Concerted Research Actions
References (32)
Show source-provided references
1. 10.1038/nmat242910.1038/nmat2429 ↗
2. 10.1021/nl203657c10.1021/nl203657c ↗
3. 10.1038/nmat186010.1038/nmat1860 ↗
4. 10.1038/nature1400410.1038/nature14004 ↗
5. 10.1063/1.347541710.1063/1.3475417 ↗
6. 10.1002/adma.20110042610.1002/adma.201100426 ↗
7. 10.1038/srep0025810.1038/srep00258 ↗
8. 10.1063/1.487095710.1063/1.4870957 ↗
9. 10.1038/nmat218410.1038/nmat2184 ↗
10. 10.1016/j.surfrep.2007.07.00110.1016/j.surfrep.2007.07.001 ↗
11. 10.1111/j.1151-2916.1981.tb10223.x10.1111/j.1151-2916.1981.tb10223.x ↗
12. 10.1103/PhysRevB.55.1395310.1103/PhysRevB.55.13953 ↗
13. 10.1002/adfm.20130116010.1002/adfm.201301160 ↗
14. 10.1103/PhysRevB.67.24541210.1103/PhysRevB.67.245412 ↗
15. 10.1063/1.312077010.1063/1.3120770 ↗
16. 10.1103/PhysRevLett.89.23720110.1103/PhysRevLett.89.237201 ↗
17. 10.1103/PhysRevLett.103.09720110.1103/PhysRevLett.103.097201 ↗
18. 10.1016/0038-1098(69)90285-310.1016/0038-1098(69)90285-3 ↗
19. 10.1039/DT972000011610.1039/DT9720000116 ↗
20. 10.1103/PhysRevB.64.21442210.1103/PhysRevB.64.214422 ↗
21. 10.1063/1.150694210.1063/1.1506942 ↗
22. 10.1116/1.57701110.1116/1.577011 ↗
23. 10.1007/s10853-006-0624-410.1007/s10853-006-0624-4 ↗
24. 10.1103/PhysRevLett.87.07610210.1103/PhysRevLett.87.076102 ↗
25. 10.1016/j.tsf.2010.12.19310.1016/j.tsf.2010.12.193 ↗
26. 10.1016/S0039-6028(99)00699-810.1016/S0039-6028(99)00699-8 ↗
27. 10.1016/0272-8842(94)90059-010.1016/0272-8842(94)90059-0 ↗
28. 10.1002/sia.336910.1002/sia.3369 ↗
29. 10.1103/PhysRev.158.60010.1103/PhysRev.158.600 ↗
30. 10.1103/PhysRevLett.91.26720110.1103/PhysRevLett.91.267201 ↗
31. 10.1007/BF0215019910.1007/BF02150199 ↗
32. 10.1023/A:101268150368610.1023/A:1012681503686 ↗