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    Structural and Magnetic Phase Transitions near Optimal Superconductivity in BaFe2(As1−xPx)2

    Ding Hu1, Xingye Lu1, Wenliang Zhang1, Huiqian Luo1, Shiliang Li1,2, Peipei Wang1, Genfu Chen1,*, Fei Han3, Shree R. Banjara4,5 et al.

    A. Sapkota4,5, A. Kreyssig4,5, A. I. Goldman4,5, Z. Yamani6, Christof Niedermayer7, Markos Skoulatos7, Robert Georgii8, T. Keller9,10, Pengshuai Wang11, Weiqiang Yu11, and Pengcheng Dai12,1,†

    • 1Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
    • 2Collaborative Innovation Center of Quantum Matter, Beijing, China
    • 3Materials Science Division, Argonne National Laboratory, Argonne, Illinois 60439, USA
    • 4Ames Laboratory, U.S. DOE, Ames, Iowa 50011, USA
    • 5Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
    • 6Canadian Neutron Beam Centre, National Research Council, Chalk River, Ontario K0J 1P0, Canada
    • 7Laboratory for Neutron Scattering, Paul Scherrer Institut, CH-5232 Villigen, Switzerland
    • 8Heinz Maier-Leibnitz Zentrum, Technische Universität München, D-85748 Garching, Germany
    • 9Max-Planck-Institut für Festkörperforschung, Heisenbergstrasse 1, D-70569 Stuttgart, Germany
    • 10Max Planck Society Outstation at the Forschungsneutronenquelle Heinz Maier-Leibnitz (MLZ), D-85747 Garching, Germany
    • 11Department of Physics, Renmin University of China, Beijing 100872, China
    • 12Department of Physics and Astronomy, Rice University, Houston, Texas 77005, USA

    • *gfchen@iphy.ac.cn
    • †pdai@rice.edu

    Phys. Rev. Lett. 114, 157002 – Published 17 April, 2015

    DOI: https://doi.org/10.1103/PhysRevLett.114.157002

    Abstract

    We use nuclear magnetic resonance (NMR), high-resolution x-ray, and neutron scattering studies to study structural and magnetic phase transitions in phosphorus-doped BaFe2(As1−xPx)2. Previous transport, NMR, specific heat, and magnetic penetration depth measurements have provided compelling evidence for the presence of a quantum critical point (QCP) near optimal superconductivity at x=0.3. However, we show that the tetragonal-to-orthorhombic structural (Ts) and paramagnetic to antiferromagnetic (AF, TN) transitions in BaFe2(As1−xPx)2 are always coupled and approach TN≈Ts≥Tc (≈29  K) for x=0.29 before vanishing abruptly for x≥0.3. These results suggest that AF order in BaFe2(As1−xPx)2 disappears in a weakly first-order fashion near optimal superconductivity, much like the electron-doped iron pnictides with an avoided QCP.

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