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Essential role of magnetic frustration in the phase diagrams of doped cobaltites

Peter P. Orth1,2,*, D. Phelan3,4, J. Zhao3, H. Zheng3, J. F. Mitchell3, C. Leighton4, and Rafael M. Fernandes5

  • 1Ames Laboratory, Ames, Iowa 50011, USA
  • 2Department of Physics and Astronomy, Iowa State University, Ames, Iowa 50011, USA
  • 3Materials Science Division, Argonne National Laboratory, Lemont, Illinois 60439, USA
  • 4Department of Chemical Engineering and Materials Science, University of Minnesota, Minneapolis, Minnesota 55455, USA
  • 5School of Physics and Astronomy, University of Minnesota, Minneapolis, Minnesota 55455, USA

  • *porth@iastate.edu

Phys. Rev. Materials 6, L071402 – Published 5 July, 2022

DOI: https://doi.org/10.1103/PhysRevMaterials.6.L071402

Abstract

Doped perovskite cobaltites (e.g., La1−xSrxCoO3) have been extensively studied for their spin-state physics, electronic inhomogeneity, and insulator-metal transitions. Ferromagnetically interacting spin-state polarons emerge at low x in the phase diagram of these compounds, eventually yielding long-range ferromagnetism. The onset of long-range ferromagnetism (x≈0.18) is substantially delayed relative to polaron percolation (x≈0.05), however, generating a troubling inconsistency. Here, Monte Carlo simulations of a disordered classical spin model are used to establish that previously ignored magnetic frustration is responsible for this effect, enabling faithful reproduction of the magnetic phase diagram.

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