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    Competing charge ordering and Jahn-Teller modes in Sr3Fe2O7: Hybrid DFT calculations and symmetry mode analysis

    Guntars Zvejnieks1, Yuri Mastrikov1, Rotraut Merkle2, and Denis Gryaznov1,*

    • *Contact author: denis.gryaznov@cfi.lu.lv

    Phys. Rev. B 112, 075118 – Published 8 August, 2025

    DOI: https://doi.org/10.1103/bqdq-5bt1

    Abstract

    Symmetry, crystal, and electronic structure properties for the second-order Ruddlesden-Popper phase of Sr3Fe2O7 are comprehensively analyzed with the help of group-theoretical approaches and hybrid DFT calculations. This study is motivated by recent findings on cooperative Jahn-Teller (JT) distortion in Sr2FeO4 [G. Zvejnieks et al., Sci. Rep. 13, 16446 (2023)] and the charge order (CO) transition in Sr3Fe2O7 [J.-H. Kim et al., Phys. Rev. Lett. 127, 097203 (2021)]. We employed the amplimodes method to identify irreducible representations (irreps) of symmetry modes responsible for phase transitions in Sr3Fe2O7. The total electronic energies were calculated using the linear combination of atomic orbitals formalism and were compared for the two distinct orthorhombic symmetries and the tetragonal phase of Sr3Fe2O7. The hybrid DFT functionals used in this analysis, PBE0, WC3PW, HSE06, r2SCANh, and r2SCAN0, represent the most important types of hybrid DFT functionals. Depending on the choice of hybrid DFT functional, we identify as the ground state either the orthorhombic space group Cmcm (CO-related symmetry mode X2−, No. 63) or SG Cmce (JT-related symmetry mode X2+, No. 64) in the relaxed atomic structures. The interplay between the cooperative effects, such as JT distortion and charge ordering, highlights the importance of selecting the appropriate hybrid DFT functional to capture relevant exchange effects accurately. The r2SCANh functional with 10% exact Hartree-Fock (HF) exchange and r2SCAN0 (with 25% exact HF exchange) yield the SG Cmcm (No.63) ground state in agreement with the recent experimental observations. We thoroughly analyze and compare the crystal structure properties calculated for the chosen hybrid DFT functionals. Furthermore, only test calculations are performed to evaluate the effect of noncollinear magnetic structures. Finally, the electronic density of states for both the orthorhombic and tetragonal structures, calculated with the r2SCANh functional, emphasizes the changes induced by the cooperative effects on the electronic properties.

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