d0 Magnetic Skyrmions in Two‐Dimensional Lattice
Source abstract
Abstract
Abstract Magnetic skyrmions are topologically protected chiral spin textures that hold great promise for information storage and processing. The current research efforts on magnetic skyrmions are exclusively based on d‐orbital magnetism, which restricts their existence in a narrow window of temperature‐external magnetic field (T‐B) phase diagram. Herein, employing first‐principles and Monte‐Carlo simulations, the work reports the identification of d0 magnetic skyrmions in 2D lattice of Tl2NO2. Arising from inversion asymmetry and strong spin‐orbit coupling compensated by ligand of heavy element, large Dzyaloshinskii–Moriya interaction is obtained in monolayer Tl2NO2. This, competed with p‐orbital exchange interaction, leads to the d0 skyrmion physics under external magnetic field. Importantly, different from d‐orbital topological magnetism, the d0 magnetic skyrmions can be stabilized in a wide window of T‐B phase diagram. The underlying physics is related to the small magnetic moment and delocalization character of d0 magnetism. Furthermore, the work also demonstrates that the d0 magnetic skyrmions are strongly coupled with ferroelectricity. These findings open a new direction for magnetic skyrmion research.
Source: crossref · Quality: baseline
Research context
OpenAlex topics: Advanced Condensed Matter Physics · Magnetic and transport properties of perovskites and related materials · Magnetic properties of thin films
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
School of Physics State Key Laboratory of Crystal Materials Shandong University Shandanan Str. 27 Jinan 250100 P. R. China
Funding
National Natural Science Foundation of China · Natural Science Foundation of Shandong Province
References (73)
Show source-provided references
1. 10.1021/acs.chemrev.0c0029710.1021/acs.chemrev.0c00297 ↗
2. 10.1016/j.physrep.2017.08.00110.1016/j.physrep.2017.08.001 ↗
3. 10.1038/nnano.2013.23310.1038/nnano.2013.233 ↗
4. 10.1038/nature0505610.1038/nature05056 ↗
5. 10.1126/science.124057310.1126/science.1240573 ↗
6. 10.1126/science.116676710.1126/science.1166767 ↗
7. 10.1038/nature0912410.1038/nature09124 ↗
8. 10.1016/0550-3213(81)90568-X10.1016/0550-3213(81)90568-X ↗
9. 10.1126/science.114579910.1126/science.1145799 ↗
10. 10.1021/acs.nanolett.7b0472210.1021/acs.nanolett.7b04722 ↗
11. 10.1039/D0MH01603A10.1039/D0MH01603A ↗
12. 10.1088/1361-6528/abe26110.1088/1361-6528/abe261 ↗
13. 10.1021/acs.nanolett.2c0310610.1021/acs.nanolett.2c03106 ↗
14. 10.1038/nmat291610.1038/nmat2916 ↗
15. 10.1038/s41563-018-0204-410.1038/s41563-018-0204-4 ↗
16. 10.1038/nmat493410.1038/nmat4934 ↗
17. 10.1103/PhysRevLett.114.17720310.1103/PhysRevLett.114.177203 ↗
18. 10.1038/nature2206010.1038/nature22060 ↗
19. 10.1038/nature2239110.1038/nature22391 ↗
20. 10.1038/s41565-018-0063-910.1038/s41565-018-0063-9 ↗
21. 10.1103/PhysRevLett.125.03720310.1103/PhysRevLett.125.037203 ↗
22. 10.1038/s41467-020-19779-610.1038/s41467-020-19779-6 ↗
23. 10.1021/acs.nanolett.2c0056410.1021/acs.nanolett.2c00564 ↗
24. 10.1021/acs.nanolett.2c0438810.1021/acs.nanolett.2c04388 ↗
25. 10.1021/acs.nanolett.2c0083610.1021/acs.nanolett.2c00836 ↗
26. 10.1103/PhysRevB.105.20542710.1103/PhysRevB.105.205427 ↗
27. 10.1021/acsnano.2c0854410.1021/acsnano.2c08544 ↗
28. 10.1021/acs.nanolett.1c0480310.1021/acs.nanolett.1c04803 ↗
29. 10.1021/acs.nanolett.8b0331510.1021/acs.nanolett.8b03315 ↗
30. 10.1103/PhysRevB.94.21441110.1103/PhysRevB.94.214411 ↗
31. 10.1126/science.121414310.1126/science.1214143 ↗
32. 10.1038/nmat440210.1038/nmat4402 ↗
33. 10.1063/5.005779410.1063/5.0057794 ↗
34. 10.1038/430630a10.1038/430630a ↗
35. 10.1016/j.solidstatesciences.2004.11.01210.1016/j.solidstatesciences.2004.11.012 ↗
36. 10.1021/nl070198m10.1021/nl070198m ↗
37. 10.1021/acs.jpcc.1c0695910.1021/acs.jpcc.1c06959 ↗
38. 10.1021/nl902073310.1021/nl9020733 ↗
39. 10.1063/5.009352910.1063/5.0093529 ↗
40. 10.1038/s41524-022-00737-310.1038/s41524-022-00737-3 ↗
41. 10.1038/ncomms1495610.1038/ncomms14956 ↗
42. 10.1103/PhysRevB.101.18440110.1103/PhysRevB.101.184401 ↗
43. 10.1103/PhysRevB.93.13440710.1103/PhysRevB.93.134407 ↗
44. 10.1063/1.513302210.1063/1.5133022 ↗
45. 10.1103/PhysRevB.98.14441110.1103/PhysRevB.98.144411 ↗
46. 10.1103/PhysRevB.101.18442610.1103/PhysRevB.101.184426 ↗
47. 10.1103/PhysRevB.103.14410110.1103/PhysRevB.103.144101 ↗
48. 10.1103/PhysRev.120.9110.1103/PhysRev.120.91 ↗
49. 10.1103/PhysRevLett.44.153810.1103/PhysRevLett.44.1538 ↗
50. 10.1103/PhysRevB.102.22040910.1103/PhysRevB.102.220409 ↗
51. 10.1103/PhysRevB.93.17440310.1103/PhysRevB.93.174403 ↗
52. 10.1103/PhysRevB.106.09440310.1103/PhysRevB.106.094403 ↗
53. 10.1021/nn204667z10.1021/nn204667z ↗
54. 10.1038/nnano.2013.2910.1038/nnano.2013.29 ↗
55. 10.1021/nl400107k10.1021/nl400107k ↗
56. 10.1021/acs.nanolett.7b0103510.1021/acs.nanolett.7b01035 ↗
57. 10.1063/1.503803710.1063/1.5038037 ↗
58. 10.1063/1.338234410.1063/1.3382344 ↗
59. 10.1103/PhysRevB.54.1116910.1103/PhysRevB.54.11169 ↗
60. 10.1103/PhysRevB.50.1795310.1103/PhysRevB.50.17953 ↗
61. 10.1103/PhysRevLett.77.386510.1103/PhysRevLett.77.3865 ↗
62. 10.1103/PhysRevB.13.518810.1103/PhysRevB.13.5188 ↗
63. 10.1103/PhysRevLett.115.26721010.1103/PhysRevLett.115.267210 ↗
64. 10.1088/0953-8984/21/39/39550210.1088/0953-8984/21/39/395502 ↗
65. 10.1021/acs.jpclett.8b0365410.1021/acs.jpclett.8b03654 ↗
66. 10.1038/s41586-018-0336-310.1038/s41586-018-0336-3 ↗
67. 10.1093/nsr/nwz16910.1093/nsr/nwz169 ↗
68. 10.1063/1.132967210.1063/1.1329672 ↗
69. 10.1103/PhysRevB.97.20511210.1103/PhysRevB.97.205112 ↗
70. 10.1038/s41535-020-00287-110.1038/s41535-020-00287-1 ↗
71. 10.1103/PhysRev.115.210.1103/PhysRev.115.2 ↗
72. 10.1038/s41524-022-00809-410.1038/s41524-022-00809-4 ↗
73. 10.1088/0022-3719/19/14/02010.1088/0022-3719/19/14/020 ↗