Coexistence of Superconductivity and Magnetism in MoSr2RCu2O8 (R=rare-earth, Mo-1212)
| dc.creator | Felner, I. | |
| dc.creator | Galstyan, E. | |
| dc.creator | Asulin, I. | |
| dc.creator | Sharoni, A. | |
| dc.creator | Millo, O. | |
| dc.date | 2003-08-05 | |
| dc.date.accessioned | 2026-07-07T02:52:46Z | |
| dc.date.available | 2026-07-07T02:52:46Z | |
| dc.description | The properties of the MoSr2RCu2O8 (R=rare earth) system are found to systematically change with the contraction of the R ions. For the light R ions (La-Nd) the samples are paramagnetic down to 5 K, whereas in the intermediate range (Sm-Tb), the Mo sublattice orders antiferromagnetically at TN, ranging from 11 to 24 K. For the heavy R ions, Ho-Tm and Y, superconductivity appears at TC in the range 19-27 K and antiferromagnetism sets in at TN < TC. This latter behavior resembles most of the magneto-superconductors, but is in sharp contrast to the iso-structural RuSr2RCu2O8 system where TN > TC. | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0308078 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0308078 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/21964 | |
| dc.subject | Superconductivity | |
| dc.title | Coexistence of Superconductivity and Magnetism in MoSr2RCu2O8 (R=rare-earth, Mo-1212) | |
| dc.type | text |