journal article·2023-10-10

Exotic surface magnetotransport phenomena in the antiferromagnetic Mott insulator NiS2

Sami El-Khatib, Faisal Mustafa, Mehmet Egilmez, Bhaskar Das, Yu Tao, Moumita Maiti, Yeon Lee, Chris Leighton

Physical Review Materials· Volume 7· Issue 10
Publisher page

Abstract

The pyrite-structure transition-metal disulfide $\mathrm{Ni}{\mathrm{S}}2$ is in principle a model cubic antiferromagnetic Mott insulator that can be doped through insulator-metal transitions with both electrons and holes (in ${\mathrm{Ni}}1--x{\mathrm{Cu}}x{\mathrm{S}}2$ and ${\mathrm{Ni}}1--x{\mathrm{Co}}x{\mathrm{S}}2$), eventually inducing superconductivity and ferromagnetism, respectively. Magnetism and transport have proven challenging to understand in $\mathrm{Ni}{\mathrm{S}}2$, however. The antiferromagnetic spin structure below $\ensuremath{\sim}39\phantom{\rule{0.16em}{0ex}}\mathrm{K}$ is complex due to frustration, while unexplained weak ferromagnetism emerges below $\ensuremath{\sim}30\phantom{\rule{0.16em}{0ex}}\mathrm{K}$. Surface conduction is also now understood to dominate in $\mathrm{Ni}{\mathrm{S}}2$ at low temperatures, raising questions about the interpretation of decades of prior data. Here, we present a complete study of the surface magnetotransport phenomena that emerge at low temperatures in high-quality single-crystal $\mathrm{Ni}{\mathrm{S}}2$, which turn out to be strikingly rich. On cooling, isotropic magnetoresistance due to a field-induced shift of the first-order weak ferromagnetic ordering transition is first uncovered, i.e., metamagnetic magnetoresistance. At lower temperatures, larger, anisotropic magnetoresistance effects arise due to distinct switching events associated with the weak ferromagnetism. Strong evidence is presented that this is due to a field-driven in-plane to out-of-plane reorientation of surface spins, likely correlated with surface steps and terraces. In-plane exchange bias accompanies these effects, further supporting this interpretation. At the lowest temperatures, the spin reorientation field eventually exceeds the 9-T measurement window, generating strongly field-asymmetric magnetoresistance. Some of these unusual phenomena also manifest in the Hall channel, culminating in a sizable anomalous Hall effect at low temperatures. These results significantly demystify recent magnetoresistance and magnetic microscopy observations in $\mathrm{Ni}{\mathrm{S}}2$ crystals and nanoflakes, and constitute an important step in elucidating the complex electronic and magnetic properties of this pivotal antiferromagnetic Mott insulator.
Source: openalex_inverted_index · Quality: baseline

Research context

OpenAlex topics: Magnetic and transport properties of perovskites and related materials · Advanced Condensed Matter Physics · Physics of Superconductivity and Magnetism

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

Affiliations

Department of Physics, American University of Sharjah, Sharjah PO Box 26666, United Arab Emirates

Materials Science and Engineering Program, American University of Sharjah, Sharjah PO Box 26666, United Arab Emirates

Department of Chemical Engineering and Materials Science, University of Minnesota, Minneapolis, Minnesota 55455, USA

Funding

U.S. Department of Energy · American University of Sharjah

References (52)

Show source-provided references
1. N. Mott · 1990
2. 10.1103/RevModPhys.70.103910.1103/RevModPhys.70.1039 ↗
3. 10.1103/RevModPhys.78.1710.1103/RevModPhys.78.17 ↗
4. 10.1103/PhysRevLett.21.61710.1103/PhysRevLett.21.617 ↗
5. 10.1021/ic50069a00810.1021/ic50069a008 ↗
6. S. Ogawa · Int. J. Magn. · 1974 · 5 · 349
7. 10.1063/1.32703710.1063/1.327037 ↗
8. 10.1103/PhysRevB.6.207810.1103/PhysRevB.6.2078 ↗
9. 10.1143/JPSJ.38.11510.1143/JPSJ.38.115 ↗
10. 10.1143/JPSJ.47.48410.1143/JPSJ.47.484 ↗
11. 10.1103/PhysRevB.68.09440910.1103/PhysRevB.68.094409 ↗
12. 10.1103/PhysRevB.77.11513510.1103/PhysRevB.77.115135 ↗
13. 10.1103/PhysRevB.83.03510610.1103/PhysRevB.83.035106 ↗
14. 10.7566/JPSJ.84.05370210.7566/JPSJ.84.053702 ↗
15. 10.1016/j.jmmm.2015.08.01210.1016/j.jmmm.2015.08.012 ↗
16. 10.1103/PhysRevLett.39.49410.1103/PhysRevLett.39.494 ↗
17. 10.1103/PhysRevB.21.167610.1103/PhysRevB.21.1676 ↗
18. 10.1103/PhysRevB.24.297210.1103/PhysRevB.24.2972 ↗
19. 10.1103/PhysRevMaterials.3.11540110.1103/PhysRevMaterials.3.115401 ↗
20. 10.1016/0375-9601(75)90333-310.1016/0375-9601(75)90333-3 ↗
21. 10.1103/PhysRevB.21.232810.1103/PhysRevB.21.2328 ↗
22. 10.1016/S0921-4526(97)00078-110.1016/S0921-4526(97)00078-1 ↗
23. 10.1021/cm980350910.1021/cm9803509 ↗
24. 10.1103/PhysRevB.93.02440910.1103/PhysRevB.93.024409 ↗
25. 10.1103/PhysRevB.52.355510.1103/PhysRevB.52.3555 ↗
26. 10.1103/PhysRevMaterials.5.11500310.1103/PhysRevMaterials.5.115003 ↗
27. 10.1103/PhysRevB.50.1057410.1103/PhysRevB.50.10574 ↗
28. 10.1103/PhysRevB.67.15511210.1103/PhysRevB.67.155112 ↗
29. 10.1039/c3ee43169j10.1039/c3ee43169j ↗
30. 10.1021/nl501942w10.1021/nl501942w ↗
31. 10.1021/ja509142w10.1021/ja509142w ↗
32. 10.1103/PhysRevMaterials.1.06540310.1103/PhysRevMaterials.1.065403 ↗
33. 10.1021/acsmaterialslett.0c0020710.1021/acsmaterialslett.0c00207 ↗
34. 10.1103/RevModPhys.82.304510.1103/RevModPhys.82.3045 ↗
35. 10.1088/0034-4885/75/9/09650110.1088/0034-4885/75/9/096501 ↗
36. 10.7566/JPSJ.82.10200110.7566/JPSJ.82.102001 ↗
37. 10.1038/s41586-020-2837-010.1038/s41586-020-2837-0 ↗
38. 10.1103/PhysRevB.107.08515010.1103/PhysRevB.107.085150 ↗
39. 10.1088/0953-8984/21/29/29550110.1088/0953-8984/21/29/295501 ↗
40. 10.1039/D3NR00467H10.1039/D3NR00467H ↗
41. 10.1063/1.11427810.1063/1.114278 ↗
42. 10.1063/1.357350310.1063/1.3573503 ↗
43. 10.1103/PhysRevLett.94.03720110.1103/PhysRevLett.94.037201 ↗
44. 10.1109/TMAG.1975.105878210.1109/TMAG.1975.1058782 ↗
45. 10.1103/PhysRevLett.106.07720310.1103/PhysRevLett.106.077203 ↗
46. 10.1016/S0304-8853(98)00266-210.1016/S0304-8853(98)00266-2 ↗
47. 10.1016/S0304-8853(99)00453-910.1016/S0304-8853(99)00453-9 ↗
48. 10.1063/1.161380610.1063/1.1613806 ↗
49. 10.1016/0927-0248(93)90095-K10.1016/0927-0248(93)90095-K ↗
50. 10.1021/acsami.9b0133510.1021/acsami.9b01335 ↗
51. 10.1021/acsami.3c0466210.1021/acsami.3c04662 ↗
52. 10.1038/s41578-022-00430-310.1038/s41578-022-00430-3 ↗