Coexistence of magnetic fluctuations and long-range order in the one-dimensional J1−J2 zigzag chain materials BaDy2O4 and BaHo2O4
Source abstract
Abstract
The compounds ${\mathrm{BaDy}}2{\mathrm{O}}4$ and ${\mathrm{BaHo}}2{\mathrm{O}}4$ are part of a family of frustrated systems exhibiting interesting properties, including spin-liquid-type ground states, magnetic-field-induced phases, and the coexistence of short- and long-range magnetic order, with dominant one-dimensional correlations, which can be described as Ising ${J}1\text{\ensuremath{-}}{J}2$ zigzag chains along the $c$ axis. We have investigated polycrystalline samples of ${\mathrm{BaDy}}2{\mathrm{O}}4$ and ${\mathrm{BaHo}}2{\mathrm{O}}4$ with both neutron diffraction and neutron spectroscopy, coupled to detailed crystalline electric field calculations. The latter points to site-dependent anisotropic magnetism in both materials, which is corroborated by the magnetic structures we determined. The two systems show the coexistence of two different long-range orders: two double N\'eel $\ensuremath{\uparrow}\ensuremath{\uparrow}\ensuremath{\downarrow}\ensuremath{\downarrow}$ orders in the $ab$ plane with propagation vectors ${\mathbf{k}}1=(\frac{1}{2},0,\frac{1}{2})$ and ${\mathbf{k}}2=(\frac{1}{2},\frac{1}{2},\frac{1}{2})$ for ${\mathrm{BaDy}}2{\mathrm{O}}4$, and two distinct arrangements of simple N\'eel $\ensuremath{\uparrow}\ensuremath{\downarrow}\ensuremath{\uparrow}\ensuremath{\downarrow}$ orders along the $c$ axis, both with the propagation vector ${\mathbf{k}}0=(0,0,0)$ for ${\mathrm{BaHo}}2{\mathrm{O}}4$. The order for both wave vectors in ${\mathrm{BaDy}}2{\mathrm{O}}4$ occurs at ${T}_{\mathrm{N}}=0.48\phantom{\rule{0.28em}{0ex}}\mathrm{K}$, while in ${\mathrm{BaHo}}2{\mathrm{O}}4$ the first order sets in at ${T}_{\mathrm{N}}\ensuremath{\sim}\phantom{\rule{3.33333pt}{0ex}}1.3\phantom{\rule{0.28em}{0ex}}\mathrm{K}$ and the second one has a lower ordering temperature of 0.84 K. Both compounds show extensive diffuse scattering which we successfully modeled with a one-dimensional axial next-nearest neighbor Ising (ANNNI) model. In both materials, strong diffusive scattering persists to temperatures well below where the magnetic order is fully saturated.
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.
References (43)
Show source-provided references
1. 10.1103/PhysRevB.71.14441410.1103/PhysRevB.71.144414 ↗
2. 10.1103/PhysRevB.78.18441010.1103/PhysRevB.78.184410 ↗
3. 10.1088/0953-8984/23/16/16420310.1088/0953-8984/23/16/164203 ↗
4. 10.1103/PhysRevB.84.17443510.1103/PhysRevB.84.174435 ↗
5. 10.1088/1742-6596/391/1/01208110.1088/1742-6596/391/1/012081 ↗
6. 10.1103/PhysRevB.88.02441110.1103/PhysRevB.88.024411 ↗
7. 10.1103/PhysRevB.91.05442410.1103/PhysRevB.91.054424 ↗
8. 10.1103/PhysRevB.89.22451110.1103/PhysRevB.89.224511 ↗
9. 10.1039/C5TC01607J10.1039/C5TC01607J ↗
10. 10.1103/PhysRevB.95.13443010.1103/PhysRevB.95.134430 ↗
11. 10.1143/JPSJ.81.02470810.1143/JPSJ.81.024708 ↗
12. 10.1103/PhysRevB.86.06420310.1103/PhysRevB.86.064203 ↗
13. 10.1088/0953-8984/25/25/25600110.1088/0953-8984/25/25/256001 ↗
14. 10.1103/PhysRevB.93.06040410.1103/PhysRevB.93.060404 ↗
15. 10.1103/PhysRevB.95.10444210.1103/PhysRevB.95.104442 ↗
16. 10.1103/PhysRevB.95.18443610.1103/PhysRevB.95.184436 ↗
17. 10.1103/PhysRevLett.112.01720310.1103/PhysRevLett.112.017203 ↗
18. 10.1016/0370-1573(88)90140-810.1016/0370-1573(88)90140-8 ↗
19. 10.1103/PhysRevB.75.06441310.1103/PhysRevB.75.064413 ↗
20. H.-J. Mikeska · 2004
21. 10.1103/PhysRevB.77.09440410.1103/PhysRevB.77.094404 ↗
22. 10.1103/PhysRevB.68.22442210.1103/PhysRevB.68.224422 ↗
23. 10.1088/0953-8984/18/1/02410.1088/0953-8984/18/1/024 ↗
24. 10.1016/j.progsolidstchem.2014.05.00110.1016/j.progsolidstchem.2014.05.001 ↗
25. 10.1016/j.physb.2006.05.32810.1016/j.physb.2006.05.328 ↗
26. 10.1107/S002188989800267210.1107/S0021889898002672 ↗
27. 10.1103/PhysRevB.85.12513310.1103/PhysRevB.85.125133 ↗
28. 10.1016/S0921-4526(99)01399-X10.1016/S0921-4526(99)01399-X ↗
29. 10.1016/0921-4526(93)90108-I10.1016/0921-4526(93)90108-I ↗
30. M. P. Marder · 201010.1002/9780470949955 ↗
31. 10.1103/PhysRevB.92.09441510.1103/PhysRevB.92.094415 ↗
32. 10.1103/PhysRev.59.69310.1103/PhysRev.59.693 ↗
33. 10.1107/S0365110X4900064310.1107/S0365110X49000643 ↗
34. 10.1139/P10-08110.1139/P10-081 ↗
35. 10.1139/p70-21710.1139/p70-217 ↗
36. 10.1103/PhysRevB.71.06440310.1103/PhysRevB.71.064403 ↗
37. 10.1103/PhysRevB.90.13440310.1103/PhysRevB.90.134403 ↗
38. 10.1103/PhysRevB.92.04111010.1103/PhysRevB.92.041110 ↗
39. 10.1103/PhysRevB.90.09442110.1103/PhysRevB.90.094421 ↗
40. 10.3389/fphy.2014.0004210.3389/fphy.2014.00042 ↗
41. 10.1103/PhysRevX.4.01100710.1103/PhysRevX.4.011007 ↗
42. 10.1038/nphys371010.1038/nphys3710 ↗
43. 10.1088/1742-6596/828/1/01201410.1088/1742-6596/828/1/012014 ↗