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Orientation-Driven Strong Perpendicular Magnetic Anisotropy in La0.67Sr0.33MnO3–SrIrO3 Heterostructures Orientation-Driven Strong Perpendicular Magnetic Anisotropy in La0.67Sr0.33MnO3–SrIrO3 Heterostructures AITranslate

Ningbo Institute of Materials Technology and Engineering; Yanshan University;Institute of Advanced Science Facilities; Ningbo Institute of Materials Technology and Engineering; Ningbo Institute of Materials Technology and Engineering; Ningbo Institute of Materials Technology and Engineering; Ningbo Institute of Materials Technology and Engineering; Ningbo Institute of Materials Technology and Engineering; Ningbo Institute of Materials Technology and Engineering; Ningbo Institute of Materials Technology and Engineering;Swiss Light Source, Paul Scherrer Institut;Swiss Light Source, Paul Scherrer Institut;Swiss Light Source, Paul Scherrer Institut; Yanshan University; University of Chinese Academy of Sciences; University of Chinese Academy of Sciences
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Publisher: ACS
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Abstract AITranslate

Strong perpendicular magnetic anisotropy (PMA) is crucial for high-performance spintronic devices. However, in transition-metal oxides, it is challenging to achieve an excellent PMA property (anisotropy energy, KU > 106 erg/cm3), limiting their application potential. Here, we report a pathway to achieve obvious PMA in 3d–5d [nLa0.67Sr0.33MnO3,nSrIrO3]m ([nLSMO, nSIO]m) heterostructures via the cooperation of interfacial engineering and crystal orientation. By depositing multilayers with a (110) orientation, significant PMA is observed despite the fact that the bare LSMO and (001)-oriented heterostructures show in-plane magnetic anisotropy. First-principles calculations suggest that in the (110)-oriented heterosystems, SIO exhibits a large and perpendicular single-ion anisotropy attributed to its strong spin–orbit coupling effect, which leads to the PMA through strong orbital hybridization between Mn and Ir ions at the LSMO/SIO interface. By varying thicknesses (n) of LSMO and SIO, the KU can be optimized to 4 × 106 erg/cm3. Moreover, the conductive behavior can also be drastically altered between insulation and metallicity with the n change, implying the potential for simultaneously obtaining ferromagnetic metals and insulators with sizable PMA in one oxide heterosystem. These findings highlight the importance of interfacial engineering and crystalline orientation in tuning PMA in oxides and provide a feasible route for developing high-performance oxide-based spintronic devices.

KeyWords AITranslate

perpendicular magnetic anisotropy La0.67Sr0.33MnO3SrIrO3 heterostructure spin–orbit coupling crystal orientation orbitalShow More
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DOI:https://doi.org/10.1021/acsaelm.3c00980

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Citation Information:

Strong perpendicular magnetic anisotropy (PMA) is crucial for high-performance spintronic devices. However, in transition-metal oxides, it is challenging to achieve an excellent PMA property (anisotropy energy, KU > 106 erg/cm3), limiting their application potential. Here, we report a pathway to achieve obvious PMA in 3d–5d [nLa0.67Sr0.33MnO3,nSrIrO3]m ([nLSMO, nSIO]m) heterostructures via the cooperation of interfacial engineering and crystal orientation. By depositing multilayers with a (110) orientation, significant PMA is observed despite the fact that the bare LSMO and (001)-oriented heterostructures show in-plane magnetic anisotropy. First-principles calculations suggest that in the (110)-oriented heterosystems, SIO exhibits a large and perpendicular single-ion anisotropy attributed to its strong spin–orbit coupling effect, which leads to the PMA through strong orbital hybridization between Mn and Ir ions at the LSMO/SIO interface. By varying thicknesses (n) of LSMO and SIO, the KU can be optimized to 4 × 106 erg/cm3. Moreover, the conductive behavior can also be drastically altered between insulation and metallicity with the n change, implying the potential for simultaneously obtaining ferromagnetic metals and insulators with sizable PMA in one oxide heterosystem. These findings highlight the importance of interfacial engineering and crystalline orientation in tuning PMA in oxides and provide a feasible route for developing high-performance oxide-based spintronic devices.

quote

GB/T 7714-2015 [1] Zengxing Lu, Lijie Wen, Jiatai Feng, et al. ACS Applied Electronic Materials, 2023(5). DOI:10.1021/acsaelm.3c00980.
MLA [1] Zengxing Lu, et al., ACS Applied Electronic Materials, no. 5, 2023, https://doi.org/10.1021/acsaelm.3c00980.
APA [1] Zengxing Lu, Lijie Wen, Jiatai Feng, Xuan Zheng, Bin Lao, Sheng Li, Kenan Zhao, Liguang Gong, Huali Yang, Guoxin Chen, Anna Zakharova, Cinthia Piamonteze, Milan Radovic, Xianfeng Hao, RunWei Li, & Zhiming Wang. (2023). ACS Applied Electronic Materials(5). https://doi.org/10.1021/acsaelm.3c00980
IEEE [1] Zengxing Lu, Lijie Wen, Jiatai Feng, Xuan Zheng, Bin Lao, Sheng Li, Kenan Zhao, Liguang Gong, Huali Yang, Guoxin Chen, Anna Zakharova, Cinthia Piamonteze, Milan Radovic, Xianfeng Hao, RunWei Li, and Zhiming Wang, ACS Applied Electronic Materials, no. 5, 2023, doi: 10.1021/acsaelm.3c00980. keywords: {perpendicular magnetic anisotropy La0.67Sr0.33MnO3SrIrO3 heterostructure spin–orbit coupling crystal orientation orbitalShow More}