Vortex lattice structure in BaFe2(As0.67P0.33)2 via small-angle neutron scattering

R. Morisaki-Ishii, H. Kawano-Furukawa, A. S. Cameron, L. Lemberger, E. Blackburn, A. T. Holmes, E. M. Forgan, L. M. DeBeer-Schmitt, K. Littrell, M. Nakajima, K. Kihou, C. H. Lee, A. Iyo, H. Eisaki, S. Uchida, J. S. White, C. D. Dewhurst, J. L. Gavilano, and M. Zolliker
Phys. Rev. B 90, 125116 – Published 9 September 2014

Abstract

We have observed a magnetic vortex lattice (VL) in BaFe2(As0.67P0.33)2 (BFAP) single crystals by small-angle neutron scattering. With the field along the c axis, a nearly isotropic hexagonal VL was formed in the field range from 1 to 16 T, and no symmetry changes in the VL were observed. The temperature dependence of the VL signal was measured and confirms the presence of (non-d-wave) nodes in the superconducting gap structure for measurements at 5 T and below. The nodal effects were suppressed at high fields. At low fields, a VL reorientation transition was observed between 1 and 3 T, with the VL orientation changing by 45. Below 1 T, the VL structure was strongly affected by pinning and the diffraction pattern had a fourfold symmetry. We suggest that this (and possibly also the VL reorientation) is due to pinning to defects aligned with the crystal structure, rather than being intrinsic. The temperature dependence of the scaled intensity suggests that BFAP possesses at least one full gap and one nodal gap with circular symmetry. Judging from the symmetry, the node structure should take the form of an “accidental” circular line node, which is consistent with recent angle-resolved photoemission spectroscopy results [Y. Zhang, Z. R. Ye, Q. Q. Ge, F. Chen, J. Jiang, M. Xu, B. P. Xie, and D. L. Feng, Nature Physics 8, 371 (2012).].

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  • Received 25 March 2014
  • Revised 23 July 2014

DOI:https://doi.org/10.1103/PhysRevB.90.125116

©2014 American Physical Society

Authors & Affiliations

R. Morisaki-Ishii1, H. Kawano-Furukawa1, A. S. Cameron2, L. Lemberger2,3, E. Blackburn2, A. T. Holmes2, E. M. Forgan2, L. M. DeBeer-Schmitt4, K. Littrell4, M. Nakajima5, K. Kihou6, C. H. Lee6, A. Iyo6, H. Eisaki6, S. Uchida5, J. S. White7,8, C. D. Dewhurst3, J. L. Gavilano7, and M. Zolliker9

  • 1Division of Natural/Applied Science, Graduate School of Humanities and Science, Ochanomizu University, Bunkyo-ku, Tokyo 112-8610, Japan
  • 2School of Physics and Astronomy, University of Birmingham, Birmingham B15 2TT, England, United Kingdom
  • 3Institut Laue-Langevin, Grenoble 38042, France
  • 4Neutron Sciences Directorate, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
  • 5Department of Physics, University of Tokyo, 7-3-1 Hongo, Bunkyo-ku, Tokyo 113-0033, Japan
  • 6National Institute of Advance Industrial Science and Technology, Tsukuba, Ibaraki 305-8568, Japan
  • 7Laboratory for Neutron Scattering, Paul Scherrer Institut, CH-5232 Villigen, Switzerland
  • 8Laboratory for Quantum Magnetism, Ecole Polytechnique Fédérale de Lausanne, CH-1015 Lausanne, Switzerland
  • 9Laboratory for Developments and Methods, Paul Scherrer Institute, CH-5232 Villigen, Switzerland

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Issue

Vol. 90, Iss. 12 — 15 September 2014

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