Ising magnetism and ferroelectricity in Ca$_3$CoMnO$_6$
| dc.creator | Wu, Hua | |
| dc.creator | Burnus, T. | |
| dc.creator | Hu, Z. | |
| dc.creator | Martin, C. | |
| dc.creator | Maignan, A. | |
| dc.creator | Cezar, J. C. | |
| dc.creator | Tanaka, A. | |
| dc.creator | Brookes, N. B. | |
| dc.creator | Khomskii, D. I. | |
| dc.creator | Tjeng, L. H. | |
| dc.date | 2008-06-10 | |
| dc.date | 2008-12-04 | |
| dc.date.accessioned | 2026-07-07T12:29:23Z | |
| dc.date.available | 2026-07-07T12:29:23Z | |
| dc.description | The origin of both the Ising chain magnetism and ferroelectricity in Ca$_3$CoMnO$_6$ is studied by $ab$ $initio$ electronic structure calculations and x-ray absorption spectroscopy. We find that Ca$_3$CoMnO$_6$ has the alternate trigonal prismatic Co$^{2+}$ and octahedral Mn$^{4+}$ sites in the spin chain. Both the Co$^{2+}$ and Mn$^{4+}$ are in the high spin state. In addition, the Co$^{2+}$ has a huge orbital moment of 1.7 $μ_B$ which is responsible for the significant Ising magnetism. The centrosymmetric crystal structure known so far is calculated to be unstable with respect to exchange striction in the experimentally observed $\uparrow\uparrow\downarrow\downarrow$ antiferromagnetic structure for the Ising chain. The calculated inequivalence of the Co-Mn distances accounts for the ferroelectricity. | |
| dc.description | 4 pages, 3 figures, PRL in press (changes made upon referees comments) | |
| dc.identifier | https://arxiv.org/abs/0806.1607 | |
| dc.identifier | http://arxiv.org/abs/0806.1607 | |
| dc.identifier | Phys. Rev. Lett. 102, 026404 (2009) | |
| dc.identifier | doi:10.1103/PhysRevLett.102.026404 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/215858 | |
| dc.subject | Materials Science | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Ising magnetism and ferroelectricity in Ca$_3$CoMnO$_6$ | |
| dc.type | text |