Charge Ordering and Incommensurate Modulations in the Metamagnetic Layered Manganese Oxysulfide Sr <sub>2</sub> MnO <sub>2</sub> Cu <sub>3.5</sub> S <sub>3</sub>

Sr<sub>2</sub>MnO<sub>2</sub>Cu<sub>3.5</sub>S<sub>3</sub> contains mixed-valent Mn ions Mn<sup>2+/3+</sup> in axially elongated MnO<sub>4</sub>S<sub>2</sub> octahedra connected via apical sulfide anions to copper-deficient antifluorite-type Cu<sub>4-δ</sub>S<sub>3</sub> layers where δ ∼ 0.5. Copper deficiency is charge-compensated by oxidation of Mn 3d states resulting in mixed-valency. The compound is tetragonal in <i>P</i>4/<i>mmm</i> at ambient temperatures (<i>a</i> = 4.016345(1) Å, <i>c</i> = 11.40708(5) Å). Below 190 K, superlattice reflections in diffraction data and an increase in resistivity, signal checkerboard charge-ordering of Mn<sup>2+</sup> and Mn<sup>3+</sup>. The superstructure approximates to a √2<i>a</i> × √2<i>a</i> × 2<i>c</i> expansion of the room temperature cell in space group <i>P</i>4<sub>2</sub>/<i>nmc</i>. However, satellite reflections signal a (3 + 2)D incommensurate modulation of Cu site occupancies in the Cu-deficient sulfide layers coupled with displacements of the sulfur positions; overall the superstructure below 190 K requires description in superspace group <i>P</i>4<sub>2</sub>/<i>nmc</i>(<i>a</i>,0,0)0000(0,<i>a</i>,0)00s0. Analysis of total scattering measurements along with pair distribution functions supports the charge-ordered low temperature model and reveals local order of distinct Mn sites within the higher-temperature charge-disordered regime. Below <i>T</i><sub>N</sub> = 27 K, long-range magnetic ordering is A-type antiferromagnetic with distinct moments for Mn<sup>2+</sup> and Mn<sup>3+</sup> ions directed perpendicular to the MnO<sub>2</sub> planes and ordered ferromagnetically. Long-range antiferromagnetic order results from interlayer antiferromagnetic coupling. A metamagnetic transition at 1.1 T corresponds to a change to long-range interlayer ferromagnetic ordering via a spin-reorientation of magnetic moments and is associated with a slight decrease in the charge separation between the Mn sublattices, consistent with observations on mixed-valent perovskite and Ruddlesden-Popper-type oxide manganites.

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Journal
Journal of the American Chemical Society
Published
2026-01-16
DOI
https://doi.org/10.1021/jacs.5c21494
Primary Topic
Magnetic and transport properties of perovskites and related materials
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article
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article

Charge Ordering and Incommensurate Modulations in the Metamagnetic Layered Manganese Oxysulfide Sr 2 MnO 2 Cu 3.5 S 3

J. Hadermann, David A. Keen, Robert D. Smyth, Oliver J. Rutt et al.
Journal of the American Chemical Society
Magnetic and transport properties of perovskites and related materials
article

Charge Ordering and Incommensurate Modulations in the Metamagnetic Layered Manganese Oxysulfide Sr 2 MnO 2 Cu 3.5 S 3

J. Hadermann, David A. Keen, Robert D. Smyth, Oliver J. Rutt, Catherine F. Smura, Andrew N. Fitch, David G. Free, S. J. Clarke, Murray David, Lemuel E. Crentsil
article en

Abstract

Sr<sub>2</sub>MnO<sub>2</sub>Cu<sub>3.5</sub>S<sub>3</sub> contains mixed-valent Mn ions Mn<sup>2+/3+</sup> in axially elongated MnO<sub>4</sub>S<sub>2</sub> octahedra connected via apical sulfide anions to copper-deficient antifluorite-type Cu<sub>4-δ</sub>S<sub>3</sub> layers where δ ∼ 0.5. Copper deficiency is charge-compensated by oxidation of Mn 3d states resulting in mixed-valency. The compound is tetragonal in <i>P</i>4/<i>mmm</i> at ambient temperatures (<i>a</i> = 4.016345(1) Å, <i>c</i> = 11.40708(5) Å). Below 190 K, superlattice reflections in diffraction data and an increase in resistivity, signal checkerboard charge-ordering of Mn<sup>2+</sup> and Mn<sup>3+</sup>. The superstructure approximates to a √2<i>a</i> × √2<i>a</i> × 2<i>c</i> expansion of the room temperature cell in space group <i>P</i>4<sub>2</sub>/<i>nmc</i>. However, satellite reflections signal a (3 + 2)D incommensurate modulation of Cu site occupancies in the Cu-deficient sulfide layers coupled with displacements of the sulfur positions; overall the superstructure below 190 K requires description in superspace group <i>P</i>4<sub>2</sub>/<i>nmc</i>(<i>a</i>,0,0)0000(0,<i>a</i>,0)00s0. Analysis of total scattering measurements along with pair distribution functions supports the charge-ordered low temperature model and reveals local order of distinct Mn sites within the higher-temperature charge-disordered regime. Below <i>T</i><sub>N</sub> = 27 K, long-range magnetic ordering is A-type antiferromagnetic with distinct moments for Mn<sup>2+</sup> and Mn<sup>3+</sup> ions directed perpendicular to the MnO<sub>2</sub> planes and ordered ferromagnetically. Long-range antiferromagnetic order results from interlayer antiferromagnetic coupling. A metamagnetic transition at 1.1 T corresponds to a change to long-range interlayer ferromagnetic ordering via a spin-reorientation of magnetic moments and is associated with a slight decrease in the charge separation between the Mn sublattices, consistent with observations on mixed-valent perovskite and Ruddlesden-Popper-type oxide manganites.

Journal of the American Chemical SocietyVol. 148(3)
Rutherford Appleton Laboratory (GB), University of Antwerp (BE), European Synchrotron Radiation Facility (FR), University of Oxford (GB)
Openalex Percentile: Top 87%
Magnetic and transport properties of perovskites and related materials
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