Two-magnon Raman scattering from the Cu3O4 layers in (Sr,Ba)2Cu3O4Cl2
| dc.creator | Holmlund, J. | |
| dc.creator | Knee, C. S. | |
| dc.creator | Andreasson, J. | |
| dc.creator | Granath, M. | |
| dc.creator | Litvinchuk, A. P. | |
| dc.creator | Borjesson, L. | |
| dc.date | 2008-04-11 | |
| dc.date | 2009-02-13 | |
| dc.date.accessioned | 2026-07-07T12:40:47Z | |
| dc.date.available | 2026-07-07T12:40:47Z | |
| dc.description | (Sr$_{2}$,Ba$_{2}$)Cu$_{3}$O$_{4}$Cl$_{2}$ are antiferromagnetic insulators which are akin to the parent compounds of the cuprate superconductors but with two distinct magnetic ordering temperatures related to two magnetic Cu$_{I}$ and Cu$_{II}$ spin sublattices. Here we present a study of these materials by means of Raman spectroscopy. Following the temperature and polarization dependence of the data we readily identify two distinct features at around 3000 cm$^{-1}$ and 300 cm$^{-1}$ that are related to two-magnon scattering from the two sublattices. The estimated spin-exchange coupling constants for the Cu$_{I}$ and Cu$_{II}$ sublattices are found to be J$_{I}\sim$139-143(132-136) meV and J$_{II}\sim$14(11) meV for Sr(Ba) compounds. Moreover, we observe modes at around 480 and 445 cm$^{-1}$ for the Sr and Ba containing samples respectively, that disappears at the ordering temperature of the Cu$_{II}$. We argue that this modes may also be of magnetic origin and possibly related to interband transitions between the Cu$_{I}$-Cu$_{II}$ sublattices. | |
| dc.description | 7 pages, 8 figures | |
| dc.identifier | https://arxiv.org/abs/0804.1859 | |
| dc.identifier | http://arxiv.org/abs/0804.1859 | |
| dc.identifier | PRB 79, 085109 (2009) | |
| dc.identifier | doi:10.1103/PhysRevB.79.085109 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/219551 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.subject | Superconductivity | |
| dc.title | Two-magnon Raman scattering from the Cu3O4 layers in (Sr,Ba)2Cu3O4Cl2 | |
| dc.type | text |