Low-temperature resistivity of single crystals YBa_2Cu_3O_{6+x} in the normal state
| dc.creator | Gantmakher, V. F. | |
| dc.creator | Kozeeva, L. P. | |
| dc.creator | Lavrov, A. N. | |
| dc.creator | Pushin, D. A. | |
| dc.creator | Shovkun, D. V. | |
| dc.creator | Tsydynzhapov, G. E. | |
| dc.creator | . | |
| dc.date | 1997-05-20 | |
| dc.date | 1998-10-19 | |
| dc.date.accessioned | 2026-07-07T09:02:41Z | |
| dc.date.available | 2026-07-07T09:02:41Z | |
| dc.description | A scan of the superconductor -- nonsuperconductor transformation in single crystals YBa_2Cu_3O_{6+x} (x about 0.37) was done in two alternative ways, namely, by applying the magnetic field and by reducing the hole concentration through the oxygen rearrangement. The in-plane normal-state resistivity ρ_{ab} obtained in both cases was quite similar; its temperature dependence can be fitted by logarithmic law in the temperature range of almost two decades. However, a different representation of the σ_{ab}=1/ρ_{ab} by a power law typical for a 3D-material near a metal -- insulator transition is also plausible. The vertical conductivity σ_c=1/ρ_c followed the power law and neither σ_c(T), nor ρ_c(T) could be fitted by log(T). It follows from the ρ_c measurements that the transformation at T=0 is split into two transitions: superconductor -- normal-metal and normal-metal -- insulator. In our samples, they are distanced in the oxygen content by Δx\approx0.025. | |
| dc.description | 5 pages, LaTeX, 3 postscript figures. Figures were embedded into text; no contents were changed | |
| dc.identifier | https://arxiv.org/abs/cond-mat/9705197 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/9705197 | |
| dc.identifier | Pis'ma v ZhETF, 65, 834 (1997) | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/148723 | |
| dc.subject | Superconductivity | |
| dc.subject | Strongly Correlated Electrons | |
| dc.title | Low-temperature resistivity of single crystals YBa_2Cu_3O_{6+x} in the normal state | |
| dc.type | text |