Local-Ising-type magnetic order and metamagnetism in the rare-earth pyrogermanate Er2Ge2O7
Source abstract
Abstract
The recent discoveries of proximate quantum spin-liquid compounds and their potential application in quantum computing informs the search for new candidate materials for quantum spin-ice and spin-liquid physics. While the majority of such work has centered on members of the pyrochlore family due to their inherently frustrated linked tetrahedral structure, the rare-earth pyrogermanates also show promise for possible frustrated magnetic behavior. With the familiar stoichiometry ${R}2{\mathrm{Ge}}2{\mathrm{O}}7$, these compounds generally have tetragonal symmetry with a rare-earth sublattice built of a spiral of alternating edge and corner-sharing rare-earth site triangles. Studies on ${\mathrm{Dy}}2{\mathrm{Ge}}2{\mathrm{O}}7$ and ${\mathrm{Ho}}2{\mathrm{Ge}}2{\mathrm{O}}7$ have shown tunable low temperature antiferromagnetic order, a high frustration index, and spin-ice-like dynamics. Here we use neutron diffraction to study magnetic order in ${\mathrm{Er}}2{\mathrm{Ge}}2{\mathrm{O}}7$ (space group $P{4}1{2}12$) and find the lowest yet Ne\'el temperature in the pyrogermanates of 1.15 K. Using neutron powder diffraction, we find the magnetic structure to order with $k=(0,0,0)$ ordering vector, magnetic space group symmetry $P{4}1^{{}^{\ensuremath{'}}}{2}1{2}^{{}^{\ensuremath{'}}}$, and a refined Er moment of $m=8.1\phantom{\rule{0.28em}{0ex}}{\ensuremath{\mu}}B$ near the expected value for the ${\mathrm{Er}}3+$ free ion. Provocatively, the magnetic structure exhibits similar ``local Ising'' behavior to that seen in the pyrocholres where the Er moment points up or down along the short Er-Er bond. Upon applying a magnetic field, we find a first-order metamagnetic transition at $\ensuremath{\sim}0.35\phantom{\rule{0.16em}{0ex}}\mathrm{T}$ to a lower symmetry $P{2}1^{{}^{\ensuremath{'}}}{2}1^{{}^{\ensuremath{'}}}2$ structure. This magnetic transition involves an inversion of Er moments aligned antiparallel to the applied field describing a class I spin-flip-type transition, indicating a strong local anisotropy at the Er site---reminiscent of that seen in the spin-ice pyrochlores.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Condensed Matter Physics · Iron-based superconductors research · Topological Materials and Phenomena
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (47)
Show source-provided references
1. 10.1103/PhysRev.79.35710.1103/PhysRev.79.357 ↗
2. 10.1088/0022-3719/11/23/01910.1088/0022-3719/11/23/019 ↗
3. 10.1146/annurev.ms.24.080194.00232110.1146/annurev.ms.24.080194.002321 ↗
4. 10.1103/RevModPhys.82.5310.1103/RevModPhys.82.53 ↗
5. 10.1126/science.aat202510.1126/science.aat2025 ↗
6. 10.1016/S0003-4916(02)00018-010.1016/S0003-4916(02)00018-0 ↗
7. 10.1038/nmat460410.1038/nmat4604 ↗
8. 10.1126/science.aah601510.1126/science.aah6015 ↗
9. 10.1016/j.physb.2017.01.02810.1016/j.physb.2017.01.028 ↗
10. 10.1021/jacs.7b1117910.1021/jacs.7b11179 ↗
11. 10.1103/PhysRevLett.119.22720810.1103/PhysRevLett.119.227208 ↗
12. 10.1038/nphys426410.1038/nphys4264 ↗
13. 10.1038/nphys382610.1038/nphys3826 ↗
14. 10.1103/PhysRevLett.79.255410.1103/PhysRevLett.79.2554 ↗
15. 10.1103/PhysRevB.65.05441010.1103/PhysRevB.65.054410 ↗
16. 10.1038/nature0643310.1038/nature06433 ↗
17. 10.1103/PhysRevLett.83.185410.1103/PhysRevLett.83.1854 ↗
18. 10.1088/0953-8984/10/14/00210.1088/0953-8984/10/14/002 ↗
19. 10.1126/science.106476110.1126/science.1064761 ↗
20. 10.1016/j.jallcom.2004.12.08410.1016/j.jallcom.2004.12.084 ↗
21. 10.1103/PhysRevLett.108.25720410.1103/PhysRevLett.108.257204 ↗
22. 10.1143/JPSJ.72.41110.1143/JPSJ.72.411 ↗
23. 10.1103/PhysRevLett.103.05640210.1103/PhysRevLett.103.056402 ↗
24. 10.1103/PhysRevLett.101.19640210.1103/PhysRevLett.101.196402 ↗
25. 10.1103/PhysRevB.70.10441810.1103/PhysRevB.70.104418 ↗
26. 10.1103/PhysRevLett.84.343010.1103/PhysRevLett.84.3430 ↗
27. 10.1016/0022-5088(87)90215-310.1016/0022-5088(87)90215-3 ↗
28. 10.1103/PhysRevB.77.22442310.1103/PhysRevB.77.224423 ↗
29. 10.1103/PhysRevB.78.10441110.1103/PhysRevB.78.104411 ↗
30. 10.1016/S0038-1098(98)00161-610.1016/S0038-1098(98)00161-6 ↗
31. 10.1038/3509251610.1038/35092516 ↗
32. 10.1103/PhysRevB.69.06441410.1103/PhysRevB.69.064414 ↗
33. 10.1088/0953-8984/16/11/01010.1088/0953-8984/16/11/010 ↗
34. 10.1107/S205322961402421810.1107/S2053229614024218 ↗
35. 10.1016/0921-4526(93)90108-I10.1016/0921-4526(93)90108-I ↗
36. 10.1107/S002188989400421810.1107/S0021889894004218 ↗
37. 10.1016/S0921-4526(99)01722-610.1016/S0921-4526(99)01722-6 ↗
38. 10.1107/S002188980601407510.1107/S0021889806014075 ↗
39. 10.1107/S002188981103897010.1107/S0021889811038970 ↗
40. 10.1107/S056773947600155110.1107/S0567739476001551 ↗
41. 10.1051/jphyscol:198272710.1051/jphyscol:1982727 ↗
42. 10.1038/nature0891710.1038/nature08917 ↗
43. 10.1080/0001873770010143310.1080/00018737700101433 ↗
44. 10.1143/PTP.31.110.1143/PTP.31.1 ↗
45. 10.1103/PhysRevB.85.06040110.1103/PhysRevB.85.060401 ↗
46. 10.1103/PhysRevB.95.21441910.1103/PhysRevB.95.214419 ↗
47. 10.1103/PhysRevB.94.02443610.1103/PhysRevB.94.024436 ↗