On the ferromagnetic structure of the intermetallic borocarbide TbCo2B2C
| dc.creator | ElMassalami, M. | |
| dc.creator | Moreno, R. | |
| dc.creator | Saeed, R. M. | |
| dc.creator | Chaves, F. A. B. | |
| dc.creator | Chaves, C. M. | |
| dc.creator | Takeya, H. | |
| dc.creator | Ouladdiaf, B. | |
| dc.creator | Amara, M. | |
| dc.date | 2008-12-23 | |
| dc.date.accessioned | 2026-07-07T12:21:21Z | |
| dc.date.available | 2026-07-07T12:21:21Z | |
| dc.description | Based on magnetization, specific heat, magnetostriction, and neutron diffraction studies on single-crystal TbCo2B2C, it is found out that the paramagnetic properties, down to liquid nitrogen temperatures, are well described by a Curie-Weiss behavior of the Tb+3 moments. Furthermore, below Tc= 6.3 K, the Tb-sublattice undergoes a ferromagnetic (FM) phase transition with the easy axis being along the (100) direction and, concomitantly, the unit cell undergoes a tetragonal-to-orthorhhombic distortion. For fields up to 90 kOe, no field-induced splitting of the Co 3d orbitals was observed; as such the internal field must be well below the critical value needed to polarize the Co 3d subsystem. The manifestation of a FM state in TbCo2B2C is unique among all other isomorphous borocarbides, in particular TbNi2B2C (Tn=15 K, incommensurate modulated magnetic state) even though the Tb-ions in both isomorphs have almost the same crystalline electric field properties. The difference in the magnetic modes of these Tb-based isomorphs is attributed to a difference in their exchange couplings caused by a variation in their lattice parameters and in the position of their Fermi levels. | |
| dc.description | 9 figures | |
| dc.identifier | https://arxiv.org/abs/0812.4330 | |
| dc.identifier | http://arxiv.org/abs/0812.4330 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/213337 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | On the ferromagnetic structure of the intermetallic borocarbide TbCo2B2C | |
| dc.type | text |