Current-induced domain wall motion driven by spin–orbit torque and Dzyaloshinskii–Moriya interaction in Pt/GdFeCo and Rh/GdFeCo wires
Source abstract
Abstract
We investigated current-induced domain wall motion (CIDWM) driven by spin–orbit torque and Dzyaloshinskii–Moriya interaction (DMI) in ferrimagnetic Pt/GdFeCo/SiN and Rh/GdFeCo/SiN wires with perpendicular magnetic anisotropy at room temperature. We found that CIDWM in the Pt/GdFeCo wire exhibits nearly two times smaller in critical current density and about four times larger in DW mobility compared to the Rh/GdFeCo wire. By measuring the CIDWM under a longitudinal in-plane magnetic field, the DMI constant (D) was estimated for both wires. The estimated value of D for the Pt/GdFeCo wire is approximately seven times larger than the Rh/GdFeCo wire. It indicated that the Pt/GdFeCo wire revealed the CIDWM with much higher efficiency, mainly attributed to the much larger DMI, which may come from significantly stronger interfacial heavy metal/ferrimagnet hybridization in the Pt/GdFeCo wire.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Magnetic properties of thin films · Theoretical and Computational Physics · Magnetic Properties and Applications
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Institute of Materials Science, Vietnam Academy of Science and Technology 1 , 18 Hoang Quoc Viet, Hanoi, Vietnam
Toyota Technological Institute 2 , Tempaku, Nagoya 468-8511, Japan
Funding
Vietnam Academy of Science and Technology
References (25)
Show source-provided references
1. Nanotechnology · 2009 · 20 · 21540110.1088/0957-4484/20/21/215401 ↗
2. Nat. Nanotechnol. · 2015 · 10 · 19510.1038/nnano.2015.41 ↗
3. J. Magn. Magn. Mater. · 2015 · 383 · 5010.1016/j.jmmm.2014.12.081 ↗
4. Jpn. J. Appl. Phys. · 2017 · 56 · 0802A410.7567/jjap.56.0802a4 ↗
5. J. Sci.: Adv. Mater. Devices · 2018 · 3 · 38910.1016/j.jsamd.2018.09.003 ↗
6. Science · 2008 · 320 · 19010.1126/science.1145799 ↗
7. Nat. Nanotechnol. · 2022 · 17 · 106510.1038/s41565-022-01213-1 ↗
8. Nat. Nanotechnol. · 2013 · 8 · 52710.1038/nnano.2013.102 ↗
9. Nat. Mater. · 2013 · 12 · 61110.1038/nmat3675 ↗
10. Nat. Nanotechnol. · 2014 · 10 · 22110.1038/nnano.2014.324 ↗
11. Nat. Commun. · 2014 · 5 · 391010.1038/ncomms4910 ↗
12. Phys. Rev. B · 2016 · 93 · 17442410.1103/physrevb.93.174424 ↗
13. Nat. Mater. · 2017 · 16 · 118710.1038/nmat4990 ↗
14. Phys. Rev. Lett. · 2018 · 121 · 05770110.1103/physrevlett.121.057701 ↗
15. Nat. Commun. · 2018 · 9 · 498410.1038/s41467-018-07373-w ↗
16. Nat. Nanotechnol. · 2018 · 13 · 115410.1038/s41565-018-0255-3 ↗
17. Nat. Electron. · 2020 · 3 · 3710.1038/s41928-019-0345-8 ↗
18. Mater. Adv. · 2022 · 3 · 702810.1039/d2ma00273f ↗
19. Adv. Electron. Mater. · 2023 · 9 · 220061310.1002/aelm.202200613 ↗
20. Nat. Commun. · 2014 · 5 · 465510.1038/ncomms5655 ↗
21. Europhys. Lett. · 2012 · 100 · 5700210.1209/0295-5075/100/57002 ↗
22. APL Mater. · 2022 · 10 · 09110210.1063/5.0086380 ↗
23. Phys. Rev. Lett. · 2015 · 115 · 26721010.1103/physrevlett.115.267210 ↗
24. Phys. Rev. Lett. · 2016 · 117 · 24720210.1103/physrevlett.117.247202 ↗
25. npj Comput. Mater. · 2020 · 6 · 8810.1038/s41524-020-00351-1 ↗