Thorium-doping induced superconductivity up to 56 K in Gd1-xThxFeAsO
| dc.creator | Wang, Cao | |
| dc.creator | Li, Linjun | |
| dc.creator | Chi, Shun | |
| dc.creator | Zhu, Zengwei | |
| dc.creator | Ren, Zhi | |
| dc.creator | Li, Yuke | |
| dc.creator | Wang, Yuetao | |
| dc.creator | Lin, Xiao | |
| dc.creator | Luo, Yongkang | |
| dc.creator | Jiang, Shuai | |
| dc.creator | Xu, Xiangfan | |
| dc.creator | Cao, Guanghan | |
| dc.creator | Xu, Zhu'an | |
| dc.date | 2008-04-28 | |
| dc.date | 2008-06-12 | |
| dc.date.accessioned | 2026-07-07T10:01:34Z | |
| dc.date.available | 2026-07-07T10:01:34Z | |
| dc.description | Following the discovery of superconductivity in an iron-based arsenide LaO1-xFxFeAs with a superconducting transition temperature (Tc) of 26 K[1], Tc was pushed up surprisingly to above 40 K by either applying pressure[2] or replacing La with Sm[3], Ce[4], Nd[5] and Pr[6]. The maximum Tc has climbed to 55 K, observed in SmO1-xFxFeAs[7, 8] and SmFeAsO1-x[9]. The value of Tc was found to increase with decreasing lattice parameters in LnFeAsO1-xFx (Ln stands for the lanthanide elements) at an apparently optimal doping level. However, the F- doping in GdFeAsO is particularly difficult[10,11] due to the lattice mismatch between the Gd2O2 layers and Fe2As2 layers. Here we report observation of superconductivity with Tc as high as 56 K by the Th4+ substitution for Gd3+ in GdFeAsO. The incorporation of relatively large Th4+ ions relaxes the lattice mismatch, hence induces the high temperature superconductivity. | |
| dc.description | 4 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/0804.4290 | |
| dc.identifier | http://arxiv.org/abs/0804.4290 | |
| dc.identifier | Europhysics Letters 83, 67006 (2008). | |
| dc.identifier | doi:10.1209/0295-5075/83/67006 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/168672 | |
| dc.subject | Superconductivity | |
| dc.title | Thorium-doping induced superconductivity up to 56 K in Gd1-xThxFeAsO | |
| dc.type | text |