Upper critical field and fluctuation conductivity in the critical regime of doped SmFeAsO
| dc.creator | Pallecchi, I. | |
| dc.creator | Fanciulli, C. | |
| dc.creator | Tropeano, M. | |
| dc.creator | Palenzona, A. | |
| dc.creator | Ferretti, M. | |
| dc.creator | Malagoli, A. | |
| dc.creator | Martinelli, A. | |
| dc.creator | Sheikin, I. | |
| dc.creator | Putti, M. | |
| dc.creator | Ferdeghini, C. | |
| dc.date | 2009-02-06 | |
| dc.date.accessioned | 2026-07-07T12:54:42Z | |
| dc.date.available | 2026-07-07T12:54:42Z | |
| dc.description | We measure magnetotransport of F doped SmFeAsO samples up to 28T and we extract the upper critical fields, using different criteria. In order to circumvent the problem of criterion-dependence Hc2 values, we suggest a thermodynamic estimation of the upper critical field slope dHc2/dT based on the analysis of conductivity fluctuations in the critical regime. A high field slope as large as -12T/K is thus extracted for the optimally doped sample. We find evidence of a two-dimensional lowest Landau level (LLL) scaling for applied fields larger than mu_0H_LLL=8T. Finally, we estimate the coherence length values and we observe that they progressively increase with decreasing Tc. In all cases, the coherence length values along the c axis are smaller than the interplanar distance, confirming the two-dimensional nature of superconductivity in this compound. | |
| dc.description | 14 pages, 4 figures, 3 tables Submitted to Phys.Rev.B | |
| dc.identifier | https://arxiv.org/abs/0902.1066 | |
| dc.identifier | http://arxiv.org/abs/0902.1066 | |
| dc.identifier | Phys. Rev. B 79, 104515 (2009) | |
| dc.identifier | doi:10.1103/PhysRevB.79.104515 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/224027 | |
| dc.subject | Superconductivity | |
| dc.subject | Materials Science | |
| dc.title | Upper critical field and fluctuation conductivity in the critical regime of doped SmFeAsO | |
| dc.type | text |