Observation of ferromagnetic ordering in a stable α−Co(OH)2 phase grown on a MoS2 surface
Source abstract
Abstract
Because of the potential application of $\mathrm{Co}{(\mathrm{OH})}2$ in a magnetic cooling system as a result of its superior magnetocaloric effect many people have investigated magnetic properties of $\mathrm{Co}{(\mathrm{OH})}2$. Unfortunately, most of the works have been carried out on the $\ensuremath{\beta}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase due to the fact that the $\ensuremath{\alpha}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase is very unstable and continuously transformed into the stable $\ensuremath{\beta}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase. However, in the present work, using a $\mathrm{Mo}{\mathrm{S}}2$ sheet as a two-dimensional template, we have been able to synthesize a stable $\ensuremath{\alpha}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase in addition to a $\ensuremath{\beta}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase by varying the layer thickness. It is seen that for thinner samples the $\ensuremath{\beta}$ phase, while for thicker samples $\ensuremath{\alpha}$ phase, is grown on the $\mathrm{Mo}{\mathrm{S}}2$ surface. Magnetic measurements are carried out for the samples over the temperature range from 2 to 300 K and it is seen that for the $\ensuremath{\beta}$ phase, ferromagnetic ordering with fairly large coercivity (1271 Oe) at 2 K is obtained instead of the usual antiferromagnetism. The most interesting result is the observation of ferromagnetic ordering with a transition temperature (Curie temperature) more than 100 K in the $\ensuremath{\alpha}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase. Complete saturation in the hysteresis curve under application of very low field having coercivity of $\ensuremath{\sim}162\phantom{\rule{0.16em}{0ex}}\mathrm{Oe}$ at 2 K and 60 Oe at 50 K is obtained. A thin stable $\ensuremath{\alpha}\text{\ensuremath{-}}\mathrm{Co}{(\mathrm{OH})}2$ phase grown on $\mathrm{Mo}{\mathrm{S}}2$ surface with very soft ferromagnetic ordering will be very useful as the core material in electromagnets.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Magnetic and transport properties of perovskites and related materials · Multiferroics and related materials · Advanced Condensed Matter Physics
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (43)
Show source-provided references
1. 10.1103/PhysRevB.83.09441810.1103/PhysRevB.83.094418 ↗
2. 10.1103/PhysRevB.84.23521110.1103/PhysRevB.84.235211 ↗
3. 10.1103/PhysRevB.82.18440310.1103/PhysRevB.82.184403 ↗
4. 10.1103/PhysRevB.77.22443010.1103/PhysRevB.77.224430 ↗
5. 10.1103/PhysRevB.82.02442510.1103/PhysRevB.82.024425 ↗
6. 10.1063/1.302833710.1063/1.3028337 ↗
7. 10.1063/1.335981310.1063/1.3359813 ↗
8. 10.1002/adma.20110460510.1002/adma.201104605 ↗
9. 10.1021/ja052333810.1021/ja0523338 ↗
10. 10.1021/ic052108r10.1021/ic052108r ↗
11. 10.1021/ic901167u10.1021/ic901167u ↗
12. 10.1143/JPSJ.21.272610.1143/JPSJ.21.2726 ↗
13. 10.1002/pssb.20155277110.1002/pssb.201552771 ↗
14. 10.1088/1361-648X/aa6e7710.1088/1361-648X/aa6e77 ↗
15. 10.1021/ic00063a04310.1021/ic00063a043 ↗
16. 10.1103/PhysRevB.93.18440310.1103/PhysRevB.93.184403 ↗
17. 10.1063/1.497434710.1063/1.4974347 ↗
18. 10.1063/1.489038210.1063/1.4890382 ↗
19. 10.1107/S002188986900655810.1107/S0021889869006558 ↗
20. 10.1039/c0jm04442c10.1039/c0jm04442c ↗
21. 10.1016/j.electacta.2014.07.07510.1016/j.electacta.2014.07.075 ↗
22. 10.1002/adfm.20140386310.1002/adfm.201403863 ↗
23. 10.1039/C4RA03982C10.1039/C4RA03982C ↗
24. 10.1039/c2jm31694c10.1039/c2jm31694c ↗
25. 10.1021/nn100393710.1021/nn1003937 ↗
26. 10.1016/0021-9517(89)90109-710.1016/0021-9517(89)90109-7 ↗
27. 10.1021/ja00003a01910.1021/ja00003a019 ↗
28. 10.1063/1.484553610.1063/1.4845536 ↗
29. 10.1063/1.481679110.1063/1.4816791 ↗
30. 10.1088/0022-3719/16/2/00610.1088/0022-3719/16/2/006 ↗
31. 10.1103/PhysRevLett.97.24720210.1103/PhysRevLett.97.247202 ↗
32. 10.1103/PhysRevB.83.23541110.1103/PhysRevB.83.235411 ↗
33. 10.1103/PhysRevX.6.04103810.1103/PhysRevX.6.041038 ↗
34. 10.1103/PhysRevB.88.14441110.1103/PhysRevB.88.144411 ↗
35. 10.1103/PhysRevB.88.03512610.1103/PhysRevB.88.035126 ↗
36. 10.1103/PhysRevLett.91.01720310.1103/PhysRevLett.91.017203 ↗
37. 10.1103/PhysRevLett.111.03720110.1103/PhysRevLett.111.037201 ↗
38. 10.1063/1.216180810.1063/1.2161808 ↗
39. 10.1063/1.291906510.1063/1.2919065 ↗
40. 10.1063/1.478880710.1063/1.4788807 ↗
41. 10.1063/1.169543810.1063/1.1695438 ↗
42. 10.1088/0953-8984/24/7/07600210.1088/0953-8984/24/7/076002 ↗
43. 10.1002/chem.20100066110.1002/chem.201000661 ↗