4.5 Article

Spin glass feature and exchange bias effect in metallic Pt/antiferromagnetic LaMnO3 heterostructure

Journal

JOURNAL OF PHYSICS-CONDENSED MATTER
Volume 33, Issue 28, Pages -

Publisher

IOP PUBLISHING LTD
DOI: 10.1088/1361-648X/ac0023

Keywords

manganite; heterostructure; ferromagnetism; spin glass; exchange bias

Funding

  1. National Natural Science Foundation of China [11604067, U1801049]

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By integrating Pt/LMO heterostructure, this study investigates emergent phenomena at interfaces, revealing unexpected ferromagnetic behavior, spin glass state, and exchange bias effect. The relationship among these phenomena is explained by the coupling between the spin glass and antiferromagnetic phases.
Emergent phenomena at interfaces have been investigated intensely in pursuit of the next generation spintronics. In this work, we have integrated heterostructure consisting of paramagnetic (PM) metallic Pt and antiferromagnetic (AFM) insulator LaMnO3 (LMO). High-quality Pt (3 nm)/LMO (100 nm) heterostructure has been obtained by pulsed laser deposition. The structure, lattice strain and magnetic properties of epitaxial Pt/LMO heterostructure are fully studied. Due to the high sensitivity of synchrotron radiation and the high quality of epitaxial layer, the reflection intensity of the 3 nm-thick ultrathin Pt layer and LMO layer can be detected, and then lattice strain can be calculated. The LMO layer is under relative large tensile strain (2.13%), while the Pt layer is under relative small compressive strain (-0.46%). Magnetization measurements suggest that unexpected ferromagnetic behavior is observed clearly in the PM-Pt/AFM-LMO heterostructure. Moreover, spin glass (SG) state and exchange bias (EB) is also observed in this heterostructure. SG state is observed as a result of competing magnetic orders and spin frustration at the Pt/LMO interface. The heterostructure shows the EB effect below blocking temperature (T (B)), which is much lower than the Neel temperature (T (N)) of LMO, suggesting that the EB is strongly related to the SG state. The EB originates from the coupling between the SG and AFM phases.

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