Iron(IV) oxides are strongly correlated materials with negative charge-transfer energy (negative Δ), and exhibit peculiar electronic and magnetic properties such as topological helical spin structures in the metallic cubic perovskite SrFeO3. Here, the spin structure of the layered negative-Δ insulator Sr2FeO4 was studied by powder neutron diffraction in zero field and magnetic fields up to 6.5 T. Below TN = 56 K, Sr2FeO4 adopts an elliptical cycloidal spin structure with modulated magnetic moments between 1.9 and 3.5 μB and a propagation vector k = (τ,τ, 0) with τ = 0.137. With increasing magnetic field the spin structure undergoes a spin-flop transition near 5 T. Synchrotron 57Fe-Mössbauer spectroscopy reveals that the spin spiral transforms to a ferromagnetic structure at pressures between 5 and 8 GPa, just in the pressure range where a Raman-active phonon nonintrinsic to the K2NiF4-type crystal structure vanishes. These results indicate an insulating ground state which is stabilized by a hidden structural distortion and differs from the charge disproportionation in other Fe(IV) oxides.
Description
Spiral magnetism, spin flop, and pressure-induced ferromagnetism in the negative charge-transfer-gap insulator Sr2FeO4
%0 Journal Article
%1 PhysRevB.105.054417
%A Adler, Peter
%A Reehuis, Manfred
%A Stüßer, Norbert
%A Medvedev, Sergey A.
%A Nicklas, Michael
%A Peets, Darren C.
%A Bertinshaw, Joel
%A Christensen, Christian Kolle
%A Etter, Martin
%A Hoser, Andreas
%A Schröder, Liane
%A Merz, Patrick
%A Schnelle, Walter
%A Schulz, Armin
%A Mu, Qingge
%A Bessas, Dimitrios
%A Chumakov, Aleksandr
%A Jansen, Martin
%A Felser, Claudia
%D 2022
%I American Physical Society
%J Phys. Rev. B
%K a
%N 5
%P 054417
%R 10.1103/PhysRevB.105.054417
%T Spiral magnetism, spin flop, and pressure-induced ferromagnetism in the negative charge-transfer-gap insulator Sr$_2$FeO$_4$
%U https://link.aps.org/doi/10.1103/PhysRevB.105.054417
%V 105
%X Iron(IV) oxides are strongly correlated materials with negative charge-transfer energy (negative Δ), and exhibit peculiar electronic and magnetic properties such as topological helical spin structures in the metallic cubic perovskite SrFeO3. Here, the spin structure of the layered negative-Δ insulator Sr2FeO4 was studied by powder neutron diffraction in zero field and magnetic fields up to 6.5 T. Below TN = 56 K, Sr2FeO4 adopts an elliptical cycloidal spin structure with modulated magnetic moments between 1.9 and 3.5 μB and a propagation vector k = (τ,τ, 0) with τ = 0.137. With increasing magnetic field the spin structure undergoes a spin-flop transition near 5 T. Synchrotron 57Fe-Mössbauer spectroscopy reveals that the spin spiral transforms to a ferromagnetic structure at pressures between 5 and 8 GPa, just in the pressure range where a Raman-active phonon nonintrinsic to the K2NiF4-type crystal structure vanishes. These results indicate an insulating ground state which is stabilized by a hidden structural distortion and differs from the charge disproportionation in other Fe(IV) oxides.
@article{PhysRevB.105.054417,
abstract = {Iron(IV) oxides are strongly correlated materials with negative charge-transfer energy (negative Δ), and exhibit peculiar electronic and magnetic properties such as topological helical spin structures in the metallic cubic perovskite SrFeO3. Here, the spin structure of the layered negative-Δ insulator Sr2FeO4 was studied by powder neutron diffraction in zero field and magnetic fields up to 6.5 T. Below TN = 56 K, Sr2FeO4 adopts an elliptical cycloidal spin structure with modulated magnetic moments between 1.9 and 3.5 μB and a propagation vector k = (τ,τ, 0) with τ = 0.137. With increasing magnetic field the spin structure undergoes a spin-flop transition near 5 T. Synchrotron 57Fe-Mössbauer spectroscopy reveals that the spin spiral transforms to a ferromagnetic structure at pressures between 5 and 8 GPa, just in the pressure range where a Raman-active phonon nonintrinsic to the K2NiF4-type crystal structure vanishes. These results indicate an insulating ground state which is stabilized by a hidden structural distortion and differs from the charge disproportionation in other Fe(IV) oxides.},
added-at = {2023-06-15T13:12:28.000+0200},
author = {Adler, Peter and Reehuis, Manfred and Stüßer, Norbert and Medvedev, Sergey A. and Nicklas, Michael and Peets, Darren C. and Bertinshaw, Joel and Christensen, Christian Kolle and Etter, Martin and Hoser, Andreas and Schröder, Liane and Merz, Patrick and Schnelle, Walter and Schulz, Armin and Mu, Qingge and Bessas, Dimitrios and Chumakov, Aleksandr and Jansen, Martin and Felser, Claudia},
biburl = {https://www.bibsonomy.org/bibtex/2aab05229b3a2c59258687bcd380ef9fa/ctqmat},
day = 17,
description = {Spiral magnetism, spin flop, and pressure-induced ferromagnetism in the negative charge-transfer-gap insulator Sr2FeO4},
doi = {10.1103/PhysRevB.105.054417},
interhash = {330e0ed91157f6a1e1b3c678fa926e07},
intrahash = {aab05229b3a2c59258687bcd380ef9fa},
journal = {Phys. Rev. B},
keywords = {a},
month = {02},
number = 5,
numpages = {10},
pages = 054417,
publisher = {American Physical Society},
timestamp = {2023-10-19T09:08:57.000+0200},
title = {Spiral magnetism, spin flop, and pressure-induced ferromagnetism in the negative charge-transfer-gap insulator Sr$_{\mathbf{2}}$FeO$_{\mathbf{4}}$},
url = {https://link.aps.org/doi/10.1103/PhysRevB.105.054417},
volume = 105,
year = 2022
}