Scaling of Hall Resistivity in the Mixed State of MgB2 Films
| dc.creator | Yang, Huan | |
| dc.creator | Jia, Ying | |
| dc.creator | Shan, Lei | |
| dc.creator | Zhuang, Chenggang | |
| dc.creator | Xi, X. X. | |
| dc.creator | Li, Qi | |
| dc.creator | Liu, Zikui | |
| dc.creator | Feng, Qingrong | |
| dc.creator | Wen, Hai-Hu | |
| dc.date | 2008-01-06 | |
| dc.date.accessioned | 2026-07-07T08:52:51Z | |
| dc.date.available | 2026-07-07T08:52:51Z | |
| dc.description | The longitudinal resistivity (rho_{xx}) and transverse resistivity (rho_{xy}) of MgB2 thin films in the mixed state were studied in detail. We found that the temperature dependencies of rho_{xx} and ρ_{xy} at a fixed magnetic field (H) satisfy the scaling law of $ρ_{xy}=Aρ_{xx}^β$, where the exponent beta varies around 2.0 for different fields. In the low field region (below 1T), beta maintains a constant value of 2.0 due to the weak pinning strength of the vortices, mainly from the superfluid of the pi band. When H>1T, beta drops abruptly to its lowest value at about 2T because of the proliferation of quasiparticles from the pi-band and, hence, the motion of the vortices from the superfluid of the sigma-band dominates the dissipation. As the field is increased further, the vortex pinning strength is weakened and beta increases monotonically towards 2.0 at a high field. All the results presented here are in good agreement with the expectation of the vortex physics of a multi-band superconductor. | |
| dc.identifier | https://arxiv.org/abs/0801.0838 | |
| dc.identifier | http://arxiv.org/abs/0801.0838 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/145421 | |
| dc.subject | Superconductivity | |
| dc.title | Scaling of Hall Resistivity in the Mixed State of MgB2 Films | |
| dc.type | text |