Transition Metal-Doped Boron Nitride Atomic Sheets with an Engineered Bandgap and Magnetization
Source abstract
Abstract
Controlled doping of flat atomic sheets of boron nitride (BN) can in principle break charge and spin symmetries. In contrast to graphene that oxidizes at >500 °C, due to its high melting point (ca. 2700 K) and the electrically insulating nature ( E g ∼ 5.5 eV), BN presents strong material candidature for flexible magnetic memory chips that are functional even under fire. Here, we report the transition metal (Fe and Cr) doping of BN by microwave and solvothermal methods. X-ray photoelectron spectroscopy reveals ∼17% doping by microwave (800 W) and <11% doping by the solvothermal method. Cr or Fe doping brings the bandgap down to ∼3.6 or ∼2.0 eV, respectively, for the doped BN samples. Cr doping by microwave results in intrinsic ferromagnetic ordering evident from the high Curie point (∼380 K) in contrast to orbital-mediated magnetic ordering in solvothermal Cr-doped BN systems. Fe doping raises magnetization values in particular. Spin-polarized DFT band structure calculations suggest vivid spin asymmetry caused by doping, supporting our experimental findings on doped BN samples.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Graphene research and applications · 2D Materials and Applications · ZnO doping and properties
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Physics, Indian Institute of Technology Patna, Bihar801106, India
Graduate School of Environmental Science and Research Institute for Electronic Science, Hokkaido University, Sapporo, Hokkaido060-0810, Japan
Global Innovative Center for Advanced Nanomaterials, University of Newcastle, Callaghan, NSW2308, Australia
Funding
Science and Engineering Research Board · Japan Society for the Promotion of Science
References (60)
Show source-provided references
1. 10.1126/science.110289610.1126/science.1102896 ↗
2. 10.1038/nmat184910.1038/nmat1849 ↗
3. 10.1021/acsmaterialslett.1c0065110.1021/acsmaterialslett.1c00651 ↗
4. 10.1186/s40580-022-00317-710.1186/s40580-022-00317-7 ↗
5. 10.1038/s41565-018-0157-410.1038/s41565-018-0157-4 ↗
6. 10.1002/adma.20190035310.1002/adma.201900353 ↗
7. 10.1002/adma.20210203910.1002/adma.202102039 ↗
8. 10.1039/D2CP01712A10.1039/D2CP01712A ↗
9. 10.1038/nnano.2014.8510.1038/nnano.2014.85 ↗
10. 10.1038/nmat438410.1038/nmat4384 ↗
11. 10.1088/1367-2630/16/9/09500210.1088/1367-2630/16/9/095002 ↗
12. 10.1021/acs.jpclett.2c0154010.1021/acs.jpclett.2c01540 ↗
13. 10.1038/natrevmats.2017.3310.1038/natrevmats.2017.33 ↗
14. 10.1021/acsmaterialslett.1c0010210.1021/acsmaterialslett.1c00102 ↗
15. 10.1038/s41563-019-0415-310.1038/s41563-019-0415-3 ↗
16. 10.1002/adma.20130413810.1002/adma.201304138 ↗
17. 10.1038/natrevmats.2016.9810.1038/natrevmats.2016.98 ↗
18. 10.1039/C5TC02729B10.1039/C5TC02729B ↗
19. 10.1039/C5NR04810A10.1039/C5NR04810A ↗
20. 10.1002/adom.20160020110.1002/adom.201600201 ↗
21. 10.1021/acsnano.5b0462810.1021/acsnano.5b04628 ↗
22. 10.1021/jp512314710.1021/jp5123147 ↗
23. 10.1021/acs.nanolett.8b0389510.1021/acs.nanolett.8b03895 ↗
24. 10.1002/advs.20220269510.1002/advs.202202695 ↗
25. 10.1002/adma.20190059710.1002/adma.201900597 ↗
26. 10.1016/j.cej.2022.13844710.1016/j.cej.2022.138447 ↗
27. 10.1016/j.ssi.2020.11537110.1016/j.ssi.2020.115371 ↗
28. 10.1038/s41699-020-00162-410.1038/s41699-020-00162-4 ↗
29. 10.1038/s41598-018-19496-710.1038/s41598-018-19496-7 ↗
30. 10.1038/nphoton.2015.27710.1038/nphoton.2015.277 ↗
31. 10.1038/s41578-019-0124-110.1038/s41578-019-0124-1 ↗
32. 10.1039/b918183k10.1039/b918183k ↗
33. 10.1109/LMAG.2019.295108510.1109/LMAG.2019.2951085 ↗
34. 10.1063/1.491629910.1063/1.4916299 ↗
35. 10.1186/s11671-020-03315-y10.1186/s11671-020-03315-y ↗
36. 10.1016/j.physe.2021.11485910.1016/j.physe.2021.114859 ↗
37. 10.1103/PhysRevB.86.04545910.1103/PhysRevB.86.045459 ↗
38. 10.1103/PhysRevLett.108.20680210.1103/PhysRevLett.108.206802 ↗
39. 10.1007/s42247-021-00170-010.1007/s42247-021-00170-0 ↗
40. 10.1038/s41598-018-30613-410.1038/s41598-018-30613-4 ↗
41. 10.1039/C6NR09312D10.1039/C6NR09312D ↗
42. 10.1039/C5NR05960G10.1039/C5NR05960G ↗
43. 10.1002/smll.20150163210.1002/smll.201501632 ↗
44. 10.1039/C6CC03302D10.1039/C6CC03302D ↗
45. 10.1016/j.solidstatesciences.2010.05.02910.1016/j.solidstatesciences.2010.05.029 ↗
46. 10.1016/j.surfcoat.2005.02.09110.1016/j.surfcoat.2005.02.091 ↗
47. Romand M. · Analysis · 1976 · 4 · 309
48. 10.18434/T4T88K10.18434/T4T88K ↗
49. 10.1088/0022-3727/47/18/18530410.1088/0022-3727/47/18/185304 ↗
50. 10.1038/srep0590110.1038/srep05901 ↗
51. 10.1103/PhysRevB.102.09440610.1103/PhysRevB.102.094406 ↗
52. 10.1002/adfm.20140114910.1002/adfm.201401149 ↗
53. 10.1021/acs.jpcc.9b0653710.1021/acs.jpcc.9b06537 ↗
54. 10.1016/j.mtcomm.2019.10075310.1016/j.mtcomm.2019.100753 ↗
55. 10.1021/acs.jpclett.7b0327610.1021/acs.jpclett.7b03276 ↗
56. 10.1016/j.mseb.2021.11537910.1016/j.mseb.2021.115379 ↗
57. 10.1039/C6CP05495A10.1039/C6CP05495A ↗
58. 10.1016/j.physleta.2016.11.01610.1016/j.physleta.2016.11.016 ↗
59. 10.1088/1361-648X/aaff4010.1088/1361-648X/aaff40 ↗
60. 10.1007/s12648-020-01732-410.1007/s12648-020-01732-4 ↗