Frustrated Magnetism in a Potential Quantum Material Based on Spin-1/2 Co2+ Dimers
Source abstract
Abstract
The layered-triangular-based compound Rb 2 Co 2 (SeO 3 ) 3 was designed and synthesized to investigate frustrated magnetism in a Co 2+ -based system. The crystal structure consists of a planar triangular array of face-sharing Co 2+ O 6 octahedra forming dimers separated by Rb + layers. Comparison of Rb 2 Co 2 (SeO 3 ) 3 to the isostructural known compound K 2 Co 2 (SeO 3 ) 3 suggests that the larger-size Rb + spacers weaken its interlayer interactions. The magnetic entropy reveals the effective S = 1/2 nature of Co 2+ at low temperatures in this compound. A feature at around 3.4 K appears in both the magnetic data and heat capacity data in zero field, which can be sensitively tuned by applying an out-of-plane magnetic field, and it shows a substantially reduced heat capacity change than expected for a 3D magnetic ordering, suggesting competing magnetic interactions and a frustrated nature. Successive magnetization plateaus observed at low temperature indicate the rich quantum magnetism that results from replacing spins with spin dimers on the triangular lattice.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Condensed Matter Physics · Physics of Superconductivity and Magnetism · Magnetic and transport properties of perovskites and related materials
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
Department of Chemistry, Princeton University, Princeton, New Jersey 08544, United States
Department of Physics and Astronomy, Johns Hopkins University, Baltimore, Maryland 21218, United States
Department of Chemistry, Michigan State University, Lansing, Michigan 48824, United States
Funding
Gordon and Betty Moore Foundation · Basic Energy Sciences
References (38)
Show source-provided references
1. 10.1016/0025-5408(73)90167-010.1016/0025-5408(73)90167-0 ↗
2. 10.1126/science.235.4793.119610.1126/science.235.4793.1196 ↗
3. 10.1126/science.abi879410.1126/science.abi8794 ↗
4. 10.1103/PhysRevLett.68.176610.1103/PhysRevLett.68.1766 ↗
5. 10.1038/nature0891710.1038/nature08917 ↗
6. 10.1038/s41567-019-0577-610.1038/s41567-019-0577-6 ↗
7. 10.1126/sciadv.aay695310.1126/sciadv.aay6953 ↗
8. 10.1103/PhysRevLett.114.07720210.1103/PhysRevLett.114.077202 ↗
9. 10.1038/s41567-019-0594-510.1038/s41567-019-0594-5 ↗
10. 10.1103/PhysRevB.102.22443010.1103/PhysRevB.102.224430 ↗
11. 10.1126/science.107881910.1126/science.1078819 ↗
12. 10.1038/nature0473210.1038/nature04732 ↗
13. 10.1107/S205322961402421810.1107/S2053229614024218 ↗
14. 10.1107/S205327331402637010.1107/S2053273314026370 ↗
15. 10.1103/PhysRev.100.56410.1103/PhysRev.100.564 ↗
16. 10.1063/1.198459010.1063/1.1984590 ↗
17. Unpublished high-field magnetization data from Prof.CollinL Broholm group
18. 10.1103/PhysRevB.75.13441210.1103/PhysRevB.75.134412 ↗
19. 10.1103/PhysRevB.108.22440310.1103/PhysRevB.108.224403 ↗
20. 10.1088/0953-8984/16/11/02810.1088/0953-8984/16/11/028 ↗
21. 10.1103/PhysRevB.97.14440610.1103/PhysRevB.97.144406 ↗
22. 10.1143/JPSJ.70.179010.1143/JPSJ.70.1790 ↗
23. 10.1103/PhysRevLett.94.04720210.1103/PhysRevLett.94.047202 ↗
24. 10.1103/PhysRevLett.111.13720410.1103/PhysRevLett.111.137204 ↗
25. 10.1038/s41467-023-39502-510.1038/s41467-023-39502-5 ↗
26. Tari A. · 200310.1142/p254 ↗
27. 10.1103/PhysRevB.90.01440310.1103/PhysRevB.90.014403 ↗
28. 10.1103/PhysRev.131.54610.1103/PhysRev.131.546 ↗
29. 10.1103/PhysRevB.97.01440710.1103/PhysRevB.97.014407 ↗
30. 10.1143/JPSJ.72.232610.1143/JPSJ.72.2326 ↗
31. 10.1103/PhysRevLett.108.05720510.1103/PhysRevLett.108.057205 ↗
32. 10.1103/PhysRevB.95.18041110.1103/PhysRevB.95.180411 ↗
33. 10.1038/s41467-021-25567-710.1038/s41467-021-25567-7 ↗
34. 10.1103/PhysRevLett.91.10700110.1103/PhysRevLett.91.107001 ↗
35. 10.1103/PhysRevB.77.10441310.1103/PhysRevB.77.104413 ↗
36. 10.1103/PhysRevB.67.10443110.1103/PhysRevB.67.104431 ↗
37. 10.1021/ja053891p10.1021/ja053891p ↗
38. 10.1103/PhysRevMaterials.4.04440110.1103/PhysRevMaterials.4.044401 ↗