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Suppression of Superconductivity and Nematic Order in Fe1–ySe1–xSx (0 ≤ x ≤ 1; y ≤ 0.1) Crystals by Anion Height Disorder

  • Aifeng Wang*
    Aifeng Wang
    Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, United States
    *Email: [email protected]
    More by Aifeng Wang
  • Ana Milosavljevic
    Ana Milosavljevic
    Center for Solid State Physics and New Materials, Institute of Physics Belgrade, University of Belgrade, Pregrevica 118, 11080 Belgrade, Serbia
  • A. M. Milinda Abeykoon
    A. M. Milinda Abeykoon
    National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, United States
  • Valentin Ivanovski
    Valentin Ivanovski
    Vinca Institute of Nuclear Sciences, University of Belgrade, Belgrade 11001, Serbia
  • Qianheng Du
    Qianheng Du
    Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, United States
    Materials Science and Chemical Engineering Department, Stony Brook University, Stony Brook, New York 11790, United States
    More by Qianheng Du
  • Andreas Baum
    Andreas Baum
    Walther Meissner Institut, Bayerische Akademie der Wissenschaften, 85748 Garching, Germany
    Fakultät für Physik E23, Technische Universität München, 85748 Garching, Germany
    More by Andreas Baum
  • Eli Stavitski
    Eli Stavitski
    National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, United States
  • Yu Liu
    Yu Liu
    Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, United States
    More by Yu Liu
  • Nenad Lazarevic
    Nenad Lazarevic
    Center for Solid State Physics and New Materials, Institute of Physics Belgrade, University of Belgrade, Pregrevica 118, 11080 Belgrade, Serbia
  • Klaus Attenkofer
    Klaus Attenkofer
    National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, United States
  • Rudi Hackl
    Rudi Hackl
    Walther Meissner Institut, Bayerische Akademie der Wissenschaften, 85748 Garching, Germany
    Fakultät für Physik E23, Technische Universität München, 85748 Garching, Germany
    More by Rudi Hackl
  • Zoran Popovic
    Zoran Popovic
    Center for Solid State Physics and New Materials, Institute of Physics Belgrade, University of Belgrade, Pregrevica 118, 11080 Belgrade, Serbia
    Serbian Academy of Sciences and Arts, Kneza Mihaila 35, Belgrade 11000, Serbia
  • , and 
  • Cedomir Petrovic*
    Cedomir Petrovic
    Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, United States
    Materials Science and Chemical Engineering Department, Stony Brook University, Stony Brook, New York 11790, United States
    *Email: [email protected]
Cite this: Inorg. Chem. 2022, 61, 29, 11036–11045
Publication Date (Web):July 13, 2022
https://doi.org/10.1021/acs.inorgchem.2c00568
Copyright © 2022 American Chemical Society

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    Abstract

    Abstract Image

    Connections between crystal chemistry and critical temperature Tc have been in the focus of superconductivity, one of the most widely studied phenomena in physics, chemistry, and materials science alike. In most Fe-based superconductors, materials chemistry and physics conspire so that Tc correlates with the average anion height above the Fe plane, i.e., with the geometry of the FeAs4 or FeCh4 (Ch = Te, Se, or S) tetrahedron. By synthesizing Fe1–ySe1–xSx (0 ≤ x ≤ 1; y ≤ 0.1), we find that in alloyed crystals Tc is not correlated with the anion height like it is for most other Fe superconductors. Instead, changes in Tc(x) and tetragonal-to-orthorhombic (nematic) transition Ts(x) upon cooling are correlated with disorder in Fe vibrations in the direction orthogonal to Fe planes, along the crystallographic c-axis. The disorder stems from the random nature of S substitution, causing deformed Fe(Se,S)4 tetrahedra with different Fe–Se and Fe–S bond distances. Our results provide evidence of Tc and Ts suppression by disorder in anion height. The connection to local crystal chemistry may be exploited in computational prediction of new superconducting materials with FeSe/S building blocks.

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    The Supporting Information is available free of charge at https://pubs.acs.org/doi/10.1021/acs.inorgchem.2c00568.

    • Experimental details, crystal structures, sample to sample reproducibility and Wilson ratio, and results of first-principles calculation (PDF)

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    Cited By

    This article is cited by 4 publications.

    1. Aifeng Wang, Lijun Wu, Qianheng Du, Muntaser Naamneh, Walber Hugo Brito, AM Milinda Abeykoon, Wojciech Radoslaw Pudelko, Jasmin Jandke, Yu Liu, Nicholas C. Plumb, Gabriel Kotliar, Vladimir Dobrosavljevic, Milan Radovic, Yimei Zhu, Cedomir Petrovic. Mooij Law Violation from Nanoscale Disorder. Nano Letters 2022, 22 (17) , 6900-6906. https://doi.org/10.1021/acs.nanolett.2c01282
    2. Y. A. Ovchenkov, D. A. Chareev, D. E. Presnov, O. S. Volkova, A. N. Vasiliev. Crossover in Low-temperature Ground State of Fe(Se,Te) Compounds. Journal of Superconductivity and Novel Magnetism 2023, 36 (1) , 183-188. https://doi.org/10.1007/s10948-022-06437-9
    3. Aifeng Wang, C Petrovic. Electron correlations in the Hc2 of Fe y Se 1−x S x (0.10 ⩽x⩽ 0.24, y⩾ 0.9). Superconductor Science and Technology 2022, 35 (11) , 115002. https://doi.org/10.1088/1361-6668/ac9161
    4. N. Lazarević, A. Baum, A. Milosavljević, L. Peis, R. Stumberger, J. Bekaert, A. Šolajić, J. Pešić, Aifeng Wang, M. Šćepanović, A. M. Milinda Abeykoon, M. V. Milošević, C. Petrovic, Z. V. Popović, R. Hackl. Evolution of lattice, spin, and charge properties across the phase diagram of FeSe 1 − x S x . Physical Review B 2022, 106 (9) https://doi.org/10.1103/PhysRevB.106.094510

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