Upper critical fields of NdFeAsO$_{0.7}$F$_{0.3}$ single crystal

ORAL

Abstract

We present measurements of the resistivity and the upper critical field $H_{c2}$ of NdFeAs O$_{0.7}$F$_{0.3}$ single crystals in strong DC and pulsed magnetic fields up to 45 T and 60 T, respectively. We found that the field scale of $H_{c2}$ is comparable to $\sim100$~T of high $T_c$ cuprates. $H_{c2}(T)$ parallel to the c-axis exhibits a pronounced upward curvature similar to what was extracted from earlier measurements on polycrystalline samples. Thus this behavior is indeed an intrinsic feature of oxypnictides, rather than manifestation of vortex lattice melting or granularity. The orientational dependence of $H_{c2}$ shows deviations from the one-band Ginzburg-Landau scaling. The mass anisotropy decreases as $T$ decreases, from 9.2 at 44 K to 5 at 34 K. We discuss to what extent different pairing scenarios can manifest themselves in the observed behavior of $H_{c2}$, using the two-band model of superconductivity. The results indicate the importance of paramagnetic effects on $H_{c2}(T)$, which may significantly reduce $H_{c2}(0)$ as compared to $H_{c2}(0)\sim200-300$ T based on extrapolations of $H_{c2}(T)$ near $T_c$ down to low temperatures.

Authors

  • J. Jaroszynski

    National High Magnetic Field Laboratory, Florida State University, Tallahassee, FL 32310, USA, NHMFL, NHMFL-Florida State University

  • F. Hunte

    NHMFL

  • Luis Balicas

    NHMFL, Florida State University, National High Magnetic Field Laboratory, Florida State University, Tallahassee-FL 32310, USA

  • Youn-jung Jo

    National High Magnetic Laboratory, NHMFL

  • I. Rai\v{c}evi\'c

    NHMFL, Dept. of Phys. \& Natl. High Magnetic Field Lab., Florida State Univ.

  • Alex Gurevich

    NHMFL, Florida State University, NHMFL-Florida State University, National High Magnetic Field Laboratory

  • D.C. Larbalestier

    NHMFL

  • Fedor Balakirev

    National High Magnetic Field Laboratory, NHMFL, NHMFL-Los Alamos National Laboratory, Los Alamos National Laboratory

  • L. Fang

    NLS CAS

  • P. Cheng

    NLS CAS

  • Y. Jia

    NLS CAS

  • Hai-Hu Wen

    Institute of Physics, Chinese Academy of Sciences, Beijing, China, NLS CAS, National Laboratory for Superconductivity, Institute of Physics and Beijing National Laboratory for Condensed Matter Physics, CAS, IOP, CAS