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Evolution of lattice, spin, and charge properties across the phase diagram of FeSe1xSx

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, and R. Hackl
Phys. Rev. B 106, 094510 – Published 19 September 2022

Abstract

A Raman scattering study covering the entire substitution range of the FeSe1xSx solid solution is presented. Data were taken as a function of sulfur concentration x for 0x1, of temperature and of scattering symmetry. All types of excitations including phonons, spins, and charges are analyzed in detail. It is observed that the energy and width of the iron-related B1g phonon mode vary continuously across the entire range of sulfur substitution. The A1g chalcogenide mode disappears above x=0.23 and reappears at a much higher energy for x=0.69. In a similar way the spectral features appearing at finite doping in A1g symmetry vary discontinuously. The magnetic excitation centered at approximately 500 cm1 disappears above x=0.23 where the A1g lattice excitations exhibit a discontinuous change in energy. The low-energy mode associated with fluctuations displays maximal intensity at the nematostructural transition and thus tracks the phase boundary.

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  • Received 9 March 2022
  • Revised 27 July 2022
  • Accepted 26 August 2022

DOI:https://doi.org/10.1103/PhysRevB.106.094510

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

N. Lazarević1,*, A. Baum2,3,*, A. Milosavljević1, L. Peis2,3,†, R. Stumberger2,3,‡, J. Bekaert4, A. Šolajić1, J. Pešić1, Aifeng Wang5, M. Šćepanović1, A. M. Milinda Abeykoon6, M. V. Milošević4, C. Petrovic7, Z. V. Popović1,8, and R. Hackl2,3,9

  • 1Center for Solid State Physics and New Materials, Institute of Physics Belgrade, University of Belgrade, Pregrevica 118, 11080 Belgrade, Serbia
  • 2Walther Meissner Institut, Bayerische Akademie der Wissenschaften, 85748 Garching, Germany
  • 3Fakultät für Physik, Technische Universität München, 85478 Garching, Germany
  • 4Department of Physics, University of Antwerp, Groenenborgerlaan 171, B-2020 Antwerp, Belgium
  • 5School of Physics, Chongqing University, Chongqing 400044, China
  • 6National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 7Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973-5000, USA
  • 8Serbian Academy of Sciences and Arts, Kneza Mihaila 35, 11000 Belgrade, Serbia
  • 9IFW Dresden, Helmholtzstr. 20, 01069 Dresden, Germany

  • *These authors contributed equally to this work.
  • Present Address: IFW Dresden, Helmholtzstr. 20, 01069 Dresden, Germany.
  • Present Address: Robert Bosch GmbH, Robert-Bosch-Platz 1, 70839 Gerlingen, Germany.

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Vol. 106, Iss. 9 — 1 September 2022

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