Full metadata record
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Her, J. L. | en_US |
dc.contributor.author | Kohama, Y. | en_US |
dc.contributor.author | Matsuda, Y. H. | en_US |
dc.contributor.author | Kindo, K. | en_US |
dc.contributor.author | Yang, W-H | en_US |
dc.contributor.author | Chareev, D. A. | en_US |
dc.contributor.author | Mitrofanova, E. S. | en_US |
dc.contributor.author | Volkova, O. S. | en_US |
dc.contributor.author | Vasiliev, A. N. | en_US |
dc.contributor.author | Lin, J-Y | en_US |
dc.date.accessioned | 2015-07-21T08:29:29Z | - |
dc.date.available | 2015-07-21T08:29:29Z | - |
dc.date.issued | 2015-04-01 | en_US |
dc.identifier.issn | 0953-2048 | en_US |
dc.identifier.uri | http://dx.doi.org/10.1088/0953-2048/28/4/045013 | en_US |
dc.identifier.uri | http://hdl.handle.net/11536/124489 | - |
dc.description.abstract | The electric resistivity of single crystalline Fe-based superconductors FeSe and FeSe0.33Te0.67 was measured in pulsed magnetic fields up to 55 T. Te-doped iron selenide, FeSe0.33Te0.67, shows rather isotropic behavior in both magnetoresistance (MR) and upper critical fields (H-c2(perpendicular to)(0)/H-c2(parallel to)(0) = 48 T/42 T similar to 1.14), when an external magnetic field is applied parallel and perpendicular to the crystallographic c-axis. These isotropic behaviors are frequently observed in an iron-based superconductor, and the isotropy in H-c2 can likely be described by the Pauli effect. In contrast, our measurements elucidate that the undoped iron selenide, FeSe, exhibits a clear anisotropy in both MR and H-c2 (H-c2(perpendicular to)(0)/H-c2(parallel to)(0) = 27 T/15 T similar to 1.8). This behavior occurs because the clean in-plane conduction (RRR = 35) allows to form a closed electron orbit within the two-dimensional Fermi sheets only for the magnetic field parallel to the c-axis, which results in an appearance of an intrinsic (orbital-effect limited) upper critical field for the undoped FeSe. Doping of Te breaks the clean in-plane conduction and leads to a crossover from an orbital limit dominating behavior to a Pauli limit dominating one. | en_US |
dc.language.iso | en_US | en_US |
dc.subject | superconductivity phase diagrams | en_US |
dc.subject | transition temperature variations | en_US |
dc.subject | phase diagrams | en_US |
dc.subject | pnictides and chalcogenides | en_US |
dc.title | Anisotropy in the upper critical field of FeSe and FeSe0.33Te0.67 single crystals | en_US |
dc.type | Article | en_US |
dc.identifier.doi | 10.1088/0953-2048/28/4/045013 | en_US |
dc.identifier.journal | SUPERCONDUCTOR SCIENCE & TECHNOLOGY | en_US |
dc.citation.volume | 28 | en_US |
dc.contributor.department | 物理研究所 | zh_TW |
dc.contributor.department | Institute of Physics | en_US |
dc.identifier.wosnumber | WOS:000351055500019 | en_US |
dc.citation.woscount | 0 | en_US |
Appears in Collections: | Articles |