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Phase transitions of LaMnO3 and SrRuO3 from DFT+U based machine learning force fields simulations

Thies Jansen, Geert Brocks, and Menno Bokdam
Phys. Rev. B 108, 235122 – Published 5 December 2023

Abstract

Perovskite oxides are known to exhibit many magnetic, electronic, and structural phases as function of doping and temperature. These materials are theoretically frequently investigated by the DFT+U method, typically in their ground state structure at T=0. We show that by combining machine learning force fields (MLFFs) and DFT+U based molecular dynamics, it becomes possible to investigate the crystal structure of complex oxides as function of temperature and U. Here, we apply this method to the magnetic transition metal compounds LaMnO3 and SrRuO3. We show that the structural phase transition from orthorhombic to cubic in LaMnO3, which is accompanied by the suppression of a Jahn-Teller distortion, can be simulated with an appropriate choice of U. For SrRuO3, we show that the sequence of orthorhombic to tetragonal to cubic crystal phase transitions can be described with great accuracy. We propose that the U values that correctly capture the temperature-dependent structures of these complex oxides can be identified by comparison of the MLFF simulated and experimentally determined structures.

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  • Received 9 August 2023
  • Revised 3 November 2023
  • Accepted 8 November 2023

DOI:https://doi.org/10.1103/PhysRevB.108.235122

©2023 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied PhysicsStatistical Physics & Thermodynamics

Authors & Affiliations

Thies Jansen*, Geert Brocks, and Menno Bokdam

  • Faculty of Science and Technology and MESA+ Institute for Nanotechnology, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands

  • *t.jansen@utwente.nl
  • m.bokdam@utwente.nl

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Issue

Vol. 108, Iss. 23 — 15 December 2023

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Images

  • Figure 1
    Figure 1

    Density of states (DOS) of LaMnO3 in its ground state structure, projected on the d orbitals of a single Mn atom for (top) Ueff=UJ=0 eV and (bottom) Ueff=3.5 eV. The right-hand side shows schematically the splitting of the d orbitals due to the crystal field, including the effect of the Jahn-Teller (JT) distortion.

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  • Figure 2
    Figure 2

    Results of MD simulations on LaMnO3, using machine learning force fields. (a) Lattice parameters as function of temperature, sampled at every tenth MD step (5 fs). The solid line is a moving average of 500 steps. The symbols , , and indicate the experimental a, b, and c lattice parameters, respectively, taken from Ref. [39]. (b) Moving average of bond angles as function of temperature; the symbols indicate the experimental data. (c) Moving average of bond length as function of temperature for Ueff=1,2,3, and 3.5 eV. The symbols indicate the experimental data. (d) Lattice parameters as function of temperature for Ueff=0,1, and 2 eV. (e) Definitions of the bond angles plotted in (b).

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  • Figure 3
    Figure 3

    Density of states (DOS) of SrRuO3 projected on the individual d orbitals of Ru for U=J=0 eV and U=3.5 and J=0.6 eV.

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  • Figure 4
    Figure 4

    Results of MD calculations on SrRuO3, using machine learning force fields, for the cases (a) U=J=0 eV and (b) U=2.6,J=0.6 eV. Lattice constants as function of temperature. The solid lines are a moving average of 500 MD steps. The symbols , , and indicate the experimental a, b, and c lattice parameters, respectively, taken from [40, 47].

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