Full-Scale Field-Free Magnetization Switching in Y3Fe5O12/Pt Nanostructures for Spin–Orbit Torque Applications
Source abstract
Abstract
High Resolution Image Download MS PowerPoint Slide The ability to achieve perpendicular magnetization switching via spin–orbit torques (SOTs) is a critical advance for the development of the next generation of spintronic applications. However, the use of an external magnetic field to break the mirror symmetry is typically required to facilitate current-induced magnetization switching, which poses a significant challenge for practical implementation. Here, we demonstrate the field-free magnetization switching in the Y 3 Fe 5 O 12 (YIG)/Pt heterostructure. This is achieved by introducing a lateral structure asymmetry in our devices, which can lead to an out-of-plane effective field. Our results provide an alternative solution for achieving field-free magnetization switching in nanoscale ferrimagnet-based heterostructures, thereby advancing the development of emerging SOT-based devices.
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Research context
OpenAlex topics: Magnetic properties of thin films · Magnetic Properties and Applications · Characterization and Applications of Magnetic Nanoparticles
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Institute of High Energy Physics
Chinese Academy of Sciences
Spallation Neutron Source Science Center
Ji Hua Laboratory
Department of Physics
Beijing Technology and Business University
Beijing National Laboratory for Condensed Matter Physics and Institute of Physics
Songshan Lake Material Laboratory
Funding
National Key Research and Development Program of China · Basic and Applied Basic Research Foundation of Guangdong Province · Songshan Lake Materials Laboratory · National Natural Science Foundation of China
References (38)
Show source-provided references
1. 10.1038/nphys334710.1038/nphys3347 ↗
2. 10.1038/s41467-018-05732-110.1038/s41467-018-05732-1 ↗
3. 10.1038/nphys417510.1038/nphys4175 ↗
4. 10.1103/RevModPhys.91.03500410.1103/RevModPhys.91.035004 ↗
5. 10.1126/science.121819710.1126/science.1218197 ↗
6. 10.1038/nature1030910.1038/nature10309 ↗
7. 10.1038/nmat481210.1038/nmat4812 ↗
8. 10.1103/PhysRevApplied.17.06402310.1103/PhysRevApplied.17.064023 ↗
9. 10.1063/5.007199410.1063/5.0071994 ↗
10. 10.1038/nnano.2014.9410.1038/nnano.2014.94 ↗
11. 10.1073/pnas.150747411210.1073/pnas.1507474112 ↗
12. 10.1038/nnano.2016.10910.1038/nnano.2016.109 ↗
13. 10.1038/nmat456610.1038/nmat4566 ↗
14. 10.1038/ncomms1085410.1038/ncomms10854 ↗
15. 10.1038/nnano.2016.8410.1038/nnano.2016.84 ↗
16. 10.1038/s41563-018-0041-510.1038/s41563-018-0041-5 ↗
17. 10.1038/nmat488610.1038/nmat4886 ↗
18. 10.1038/s41565-020-00826-810.1038/s41565-020-00826-8 ↗
19. 10.1016/j.eng.2021.09.01810.1016/j.eng.2021.09.018 ↗
20. 10.1002/adfm.20240101810.1002/adfm.202401018 ↗
21. 10.1088/1361-6463/ab751110.1088/1361-6463/ab7511 ↗
22. 10.1007/s11467-022-1197-710.1007/s11467-022-1197-7 ↗
23. 10.1021/acsaelm.2c0067210.1021/acsaelm.2c00672 ↗
24. 10.1021/acsnano.2c0375610.1021/acsnano.2c03756 ↗
25. 10.1103/PhysRevB.91.21443410.1103/PhysRevB.91.214434 ↗
26. 10.35848/1882-0786/ad2d7410.35848/1882-0786/ad2d74 ↗
27. 10.1103/PhysRevB.93.14440910.1103/PhysRevB.93.144409 ↗
28. 10.1063/1.512483210.1063/1.5124832 ↗
29. 10.1063/1.509803310.1063/1.5098033 ↗
30. 10.1063/1.514053010.1063/1.5140530 ↗
31. 10.1002/aelm.20230078510.1002/aelm.202300785 ↗
32. 10.1103/PhysRevApplied.10.04403810.1103/PhysRevApplied.10.044038 ↗
33. 10.1016/j.pmatsci.2015.06.00310.1016/j.pmatsci.2015.06.003 ↗
34. 10.1002/aelm.20210059010.1002/aelm.202100590 ↗
35. 10.1103/PhysRevB.93.01441410.1103/PhysRevB.93.014414 ↗
36. 10.1038/srep1182310.1038/srep11823 ↗
37. 10.1103/PhysRevB.99.10440110.1103/PhysRevB.99.104401 ↗
38. 10.1021/acs.nanolett.0c0397210.1021/acs.nanolett.0c03972 ↗