Frustrated minority spins in GeNi2O4
| dc.creator | Matsuda, M. | |
| dc.creator | Chung, J. -H. | |
| dc.creator | Park, S. | |
| dc.creator | Sato, T. J. | |
| dc.creator | Matsuno, K. | |
| dc.creator | Aruga-Katori, H. | |
| dc.creator | Takagi, H. | |
| dc.creator | Kakurai, K. | |
| dc.creator | Kamazawa, K. | |
| dc.creator | Tsunoda, Y. | |
| dc.creator | Kagomiya, I. | |
| dc.creator | Henley, C. L. | |
| dc.creator | Lee, S. -H. | |
| dc.date | 2007-08-23 | |
| dc.date.accessioned | 2026-07-07T08:25:13Z | |
| dc.date.available | 2026-07-07T08:25:13Z | |
| dc.description | Recently, two consecutive phase transitions were observed, upon cooling, in an antiferromagnetic spinel GeNi$_2$O$_4$ at $T_{N1}=12.1$ K and $T_{N2}=11.4$ K, respectively \cite{matsuno, crawford}. Using unpolarized and polarized elastic neutron scattering we show that the two transitions are due to the existence of frustrated minority spins in this compound. Upon cooling, at $T_{N1}$ the spins on the $<111>$ \kagome planes order ferromagnetically in the plane and antiferromagnetically between the planes (phase I), leaving the spins on the $<111>$ triangular planes that separate the \kagome planes frustrated and disordered. At the lower $T_{N2}$, the triangular spins also order in the $<111>$ plane (phase II). We also present a scenario involving exchange interactions that qualitatively explains the origin of the two purely magnetic phase transitions. | |
| dc.identifier | https://arxiv.org/abs/0708.3162 | |
| dc.identifier | http://arxiv.org/abs/0708.3162 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/136587 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Frustrated minority spins in GeNi2O4 | |
| dc.type | text |