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Phys. Rev. B 79, 144527 (2009) [5 pages]

Doping dependence of the upper critical field and Hall resistivity of LaFeAsO1−xFx (x=0, 0.025, 0.05, 0.07, 0.11, and 0.14)

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Y. Kohama1,2, Y. Kamihara3,4, S. A. Baily1,5, L. Civale5, S. C. Riggs6, F. F. Balakirev1, T. Atake2, M. Jaime1, M. Hirano3,4, and H. Hosono3,4
1MPA-NHMFL, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
2Materials and Structures Laboratory, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan
3ERATO-SORST, Japan Science and Technology Agency in Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan
4Frontier Research Center, Tokyo Institute of Technology, 4259 Nagatsuta-cho, Midori-ku, Yokohama 226-8503, Japan
5Superconductivity Technology Center, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
6NHMFL, Florida State University, Tallahassee, Florida 32310, USA

Received 18 August 2008; published 30 April 2009

The electrical resistivity (ρxx) and Hall resistivity (ρxy) of LaFeAsO1−xFx have been measured over a wide fluorine-doping range 0≤x≤0.14 using 60 T pulsed magnets. While the superconducting phase diagram (Tc,x) displays the classic dome-shaped structure, we find that the resistive upper critical field (Hc2) increases monotonically with decreasing fluorine concentration, with the largest Hc2≥75 T for x=0.05. This is reminiscent of the composition dependence in high-Tc cuprates and might correlate with opening of a pseudogap in the underdoped region. Furthermore, the temperature dependence of Hc2(T) for superconducting samples can be understood in terms of multiband superconductivity. ρxy data for nonsuperconducting samples show nonlinear field dependence, which is also consistent with a multicarrier scenario.

© 2009 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.79.144527
DOI:
10.1103/PhysRevB.79.144527
PACS:
74.25.Fy, 74.25.Ha, 74.62.Dh, 74.70.−b