Vortex phase diagram of Ba(Fe0.93Co0.07)2As2 single crystals
| dc.creator | Prozorov, R. | |
| dc.creator | Ni, N. | |
| dc.creator | Tanatar, M. A. | |
| dc.creator | Kogan, V. G. | |
| dc.creator | Gordon, R. T. | |
| dc.creator | Martin, C. | |
| dc.creator | Blomberg, E. C. | |
| dc.creator | Prommapan, P. | |
| dc.creator | Yan, J. Q. | |
| dc.creator | Bud'ko, S. L. | |
| dc.creator | Canfield, P. C. | |
| dc.date | 2008-10-08 | |
| dc.date.accessioned | 2026-07-07T12:27:56Z | |
| dc.date.available | 2026-07-07T12:27:56Z | |
| dc.description | Detailed measurements of the global and local electromagnetic properties of Ba(Fe$_{0.93}$Co$_{0.07}$)$_{2}$As$_{2}$ single crystals are reported. Analysis of the irreversible magnetic response provides strong evidence for similar vortex physics in this Fe-based pnictide superconductor to the high-$T_{c}$ cuprates, such as Y-Ba-Cu-O or Nd-Ce-Cu-O. In particular, we have found a nonmonotonic "fishtail" magnetization in $M(H,T=const)$ loops and its signature is also present in $M(H=const,T)$ scans. The supercurrent density is evaluated by using several techniques, including direct transport measurements. At 5 K we estimate its value to be a moderate $j \approx 2.6 \pm 0.2 \times 10^5$ A/cm$^2$. Analysis of the magnetic relaxation is consistent with the collective pinning and creep models (weak pinning and fast creep) and suggests a crossover from the collective to the plastic creep regime in fields exceeding the value corresponding to the maximum in fishtail magnetization. | |
| dc.identifier | https://arxiv.org/abs/0810.1338 | |
| dc.identifier | http://arxiv.org/abs/0810.1338 | |
| dc.identifier | Phys. Rev. B 78, 224506 (2008) | |
| dc.identifier | doi:10.1103/PhysRevB.78.224506 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/215375 | |
| dc.subject | Superconductivity | |
| dc.title | Vortex phase diagram of Ba(Fe0.93Co0.07)2As2 single crystals | |
| dc.type | text |