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| Hauptseite > Publikationsdatenbank > Multiple field-induced phases in the frustrated triangular magnet Cs$_3$Fe$_2$B$_ 9$ > print |
| Hauptseite > Publikationsdatenbank > Multiple field-induced phases in the frustrated triangular magnet Cs$_3$Fe$_2$B$_ 9$ > print |
| 001 | 903596 | ||
| 005 | 20220503191449.0 | ||
| 024 | 7 | _ | |a 10.1103/PhysRevB.104.064418 |2 doi |
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| 100 | 1 | _ | |a Brüning, D. |0 0000-0001-5830-2683 |b 0 |e Corresponding author |
| 245 | _ | _ | |a Multiple field-induced phases in the frustrated triangular magnet Cs$_3$Fe$_2$B$_ 9$ |
| 260 | _ | _ | |a Woodbury, NY |c 2021 |b Inst. |
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| 520 | _ | _ | |a The recently discovered material Cs$_3$Fe$_2$Br$_9$ contains Fe$_2$Br$_9$ bi-octahedra forming triangular layers with hexagonal stacking along the $c$ axis. In contrast to isostructural Cr-based compounds, the zero-field ground state is not a nonmagnetic S=0 singlet-dimer state. Instead, the Fe$_2$Br$_9$ bi-octahedra host semiclassical S=5/2 Fe$^{3+}$ spins with a pronounced easy-axis anisotropy along c, and interestingly, the intradimer spins are ordered ferromagnetically. The high degree of magnetic frustration due to (various) competing intradimer and interdimer couplings leads to a surprisingly rich magnetic phase diagram. The zero-field ground state is already reached via an intermediate phase, and the high-field magnetization and thermal expansion data for H∥c identify 10 different ordered phases. Among them are phases with constant magnetization of 1/3, respectively 1/2, of the saturation value, and several transitions are strongly hysteretic with pronounced length changes, reflecting strong magnetoelastic coupling. |
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