Two-band superconductivity in LaFeAsO0.89F0.11 at very high magnetic fields

F. Hunte, J. Jaroszynski, A. Gurevich, D. C. Larbalestier, R. Jin, A. S. Sefat, M. A. McGuire, B. C. Sales, D. K. Christen, D. Mandrus

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Abstract

The recent synthesis of the superconductor LaFeAsO0.89F 0.11 with transition temperature Tc ≈ 26 K (refs 1-4) has been quickly followed by reports of even higher transition temperatures in related compounds: 41 K in CeFeAsO0.84F0.16 (ref. 5), 43 K in SmFeAsO0.9F0.1 (ref. 6), and 52 K in NdFeAsO 0.89F0.11 and PrFeAsO0.89F0.11 (refs 7, 8). These discoveries have generated much interest in the mechanisms and manifestations of unconventional superconductivity in the family of doped quaternary layered oxypnictides LnOTMPn (Ln: La, Pr, Ce, Sm; TM: Mn, Fe, Co, Ni; Pn: P, As), because many features of these materials set them apart from other known superconductors. Here we report resistance measurements of LaFeAsO 0.89F0.11 at high magnetic fields, up to 45 T, that show a remarkable enhancement of the upper critical field Bc2 compared to values expected from the slopes dBc2/dT ≈ 2 T K-1 near Tc, particularly at low temperatures where the deduced B c2(0) ≈ 63-65 T exceeds the paramagnetic limit. We argue that oxypnictides represent a new class of high-field superconductors with B c2 values surpassing those of Nb3Sn, MgB2 and the Chevrel phases, and perhaps exceeding the 100 T magnetic field benchmark of the high-Tc copper oxides.

Original languageEnglish
Pages (from-to)903-905
Number of pages3
JournalNature
Volume453
Issue number7197
DOIs
StatePublished - Jun 12 2008

Funding

Acknowledgements Work at the NHMFL was supported by IHRP under NSF Cooperative Agreement, by the State of Florida, by the DOE, by the NSF Focused Research Group on Magnesium Diboride (FRG), and by AFOSR. Work at ORNL was supported by the Division of Materials Sciences and Engineering, Office of Basic Energy Sciences. We are grateful for discussions with G. Boebinger, E. Hellstrom, P. Lee, J. Jiang, and C. Tarantini at the NHMFL.

FundersFunder number
IHRP
Office of Basic Energy Sciences
National Science Foundation
U.S. Department of Energy
Air Force Office of Scientific Research
Division of Materials Sciences and Engineering

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