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Realization of exchange bias control with manipulation of interfacial frustration in magnetic complex oxide heterostructures

  • Ji Zhang*
  • , Jack Yang
  • , Grace L. Causer
  • , Junjie Shi
  • , Frank Klose
  • , Jing-Kai Huang
  • , Allen Tseng
  • , Danyang Wang
  • , Xiaotao Zu
  • , Liang Qiao*
  • , Anh Pham*
  • , Sean Li*
  • *Corresponding author for this work

Research output: Journal Publications and ReviewsRGC 21 - Publication in refereed journalpeer-review

Abstract

Rich exchange bias (EB) behaviors were previously observed when ferromagnetic (FM) materials contacted a spin glass, demonstrating magnetic degrees of freedom of the coupling between the glass and FM spins. However, the correlation between the degree of magnetic spin frustration and the strength of the resulting EB is far from being understood. Here, we systematically investigate the dependency of EB on interfacial spin frustration in magnetic complex oxide heterostructures including La0.7Ca0.3MnO3/CaMnO3 (LCMO/CMO) systems. The experimental analysis revealed that the extent of interfacial spin frustration is determined by the subtle competition between different types of magnetic orders related to the glassy spin behaviors at the interface. Such spin frustration can be manipulated through strain engineering through changes in the Mn eg orbital by alternating the stacking sequence of the heterostructures. A highly tunable EB field with 95% change of strength between the highly and weakly frustrated heterostructures has been achieved. Magnetic depth profiles of the heterostructures provide convincing evidence that a magnetically depressed region always occurs in the LCMO layer at the LCMO/CMO interfaces irrespective of the stacking sequence. Finally, EB is established at the magnetic interface in the LCMO layer. © 2021 American Physical Society.
Original languageEnglish
Article number174444
JournalPhysical Review B
Volume104
Issue number17
Online published30 Nov 2021
DOIs
Publication statusPublished - 2021
Externally publishedYes

Funding

The authors would like to thank the Australian Research Council No. DP190103661 for financial support. The authors acknowledge use of facilities in the Solid State & Elemental Analysis Unit at Mark Wainwright Analytical Centre. L.Q. was supported by the National Natural Science Foundation of China (Grant No. 11774044).

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