9–13 Jul 2017
Monona Terrace Community and Convention Center
US/Central timezone

[Invited] Different nature of flux pinning in Fe-based superconductors

12 Jul 2017, 10:00
30m
Lecture Hall

Lecture Hall

Speaker

Chiara Tarantini (ASC-NHMFL, Florida State University)

Description

The Fe-based superconductors (FBS) present a large variety of compounds whose properties, including flux pinning, are affected to different extents by their crystal structures. The doped $AEFe_2As_2$ phases ($AE = Ba,Sr$) mostly show a 3D character similar to low-$T_c$ superconductors and can accept a high density of artificial pinning centers. On the contrary, the $REFeAs(O,F)$ family ($RE1111$, $RE$ rare earth element) has the highest critical temperature $T_c$ (~58 K in bulk form) among FBS and a large upper critical field anisotropy that induce properties more similar to high-$T_c$ superconductors (HTS). Here we investigated the pinning properties of Nd1111 in flux-creep regime.[1] For $H//c$ the critical current density $J_c$ can be described by standard mechanisms such as point/planar defect pinning and vortex shearing. When the field approaches the $ab$-planes two different regimes are observed at low temperatures as a consequence of the transition between 3D-Abrikosov and 2D-Josephson vortices: one is determined by the formation of a vortex staircase structure, which suppresses the $n$-value ($V \sim I^n$ ), the other one by the lock-in of the vortices parallel to the layers, which induces an increase of $n$. This is the first study on FBS showing this behavior in a full temperature, field, and angular range and demonstrates that, despite the relatively low $T_c$ and anisotropy of Nd1111 compared to HTS, this compound is substantially affected by intrinsic pinning similarly to $YBa_2Cu_3O_{7-\delta}$.

A portion of this work was performed at the National High Magnetic Field Laboratory, supported by National Science Foundation Cooperative Agreement No. DMR-1157490 and State of Florida. The research leading to these results has received funding from European Union's Seventh Framework Programme (FP7/2007-2013) under grant agreement 283141 (IRON-SEA) and supported by Strategic International Collaborative Research Program (SICORP), Japan Science and Technology Agency.

[1] Tarantini et al. Scientific Reports 6, 36047 (2016).

Author

Chiara Tarantini (ASC-NHMFL, Florida State University)

Co-authors

M. Chihara (Department of Crystalline Materials Science, Nagoya University) T. Hatano (Department of Crystalline Materials Science, Nagoya University) Prof. Bernhard Holzapfel (KIT Karlsruhe) H. Ikuta (Department of Crystalline Materials Science, Nagoya University) Prof. Paul Seidel (Institut für Festkörperphysik, Friedrich-Schiller-Universität Jena) Mr Stefan Schmidt (Institut für Festkörperphysik, Friedrich-Schiller-Universität Jena) Kazumasa Iida (Nagoya Universty) Dr Jens Haenisch (Karlsruhe Institute for Technology) Dr Fritz Kurth (Institute for Metallic Materials, IFW Dresden) Dr Jan Jaroszynski (Applied Superconductivity Center, National High Magnetic Field Laboratory, Florida State University) N. Sumiya (Department of Crystalline Materials Science, Nagoya University) David Larbalestier (National High Magnetic Field Laboratory)

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