Contrasting Magnetic Structures in the Quaternary Sulfides Ba<sub>2</sub>FeMS<sub>5</sub> (M = Sb, Bi)

Ba<sub>2</sub>FeSbS<sub>5</sub> and Ba<sub>2</sub>FeBiS<sub>5</sub> are two isostructural quaternary sulfides that crystallize in the <i>Pnma</i> space group with four formula units per unit cell. Ba<sub>2</sub>FeSbS<sub>5</sub> has lattice parameters <i>a</i> = 12.08609(3) Å, <i>b</i> = 8.83426(2) Å, and <i>c</i> = 8.89114(2) Å, and Ba<sub>2</sub>FeBiS<sub>5</sub> has <i>a</i> = 12.09610(3) Å, <i>b</i> = 8.89281(2) Å, and <i>c</i> = 8.82437(2) Å at room temperature. They comprise infinite [FeMS<sub>5</sub>]<sup>4-</sup> (M = Sb, Bi) chains, where Fe<sup>3+</sup> is present in FeS<sub>4</sub> tetrahedra and M<sup>3+</sup> ions reside in edge-sharing MS<sub>6</sub> distorted octahedra, each of which shares an edge with an FeS<sub>4</sub> tetrahedron. Powder neutron diffraction measurements confirm the presence of long-range antiferromagnetic order of the Fe<sup>3+</sup> moments in both materials, where Fe-S···S-Fe super-superexchange interactions which act along the direction of the [FeMS<sub>5</sub>]<sup>4-</sup> (M = Sb, Bi) chains are the driving force for this antiferromagnetic order. The magnetic Bragg reflections reside on a <i>k</i>-vector with <i>k</i> = (1/2 0 1/2), and the relative orientations of the moments are similar in the two cases One significant difference is that the moments are aligned along the crystallographic <i>b</i>-axis in Ba<sub>2</sub>FeSbS<sub>5</sub>, whereas in Ba<sub>2</sub>FeBiS<sub>5</sub> they lie along the longer crystallographic <i>a</i>-axis, reflecting the weak directional preference of the Fe<sup>3+</sup> moments. Furthermore, an additional incommensurately modulated ordering of the Fe<sup>3+</sup> moments is suggested for Ba<sub>2</sub>FeSbS<sub>5</sub> (but not Ba<sub>2</sub>FeBiS<sub>5</sub>) by the appearance of small additional magnetic Bragg peaks in the neutron diffraction data, which may be a consequence of greater magnetic frustration in Ba<sub>2</sub>FeSbS<sub>5</sub>.

Authors

Institutions

Publication Details

Journal
Inorganic Chemistry
Published
2024-11-25
DOI
https://doi.org/10.1021/acs.inorgchem.4c03770
Citations
1
Primary Topic
Magnetic and transport properties of perovskites and related materials
Type
article
Field-Weighted Citation Impact
0.12

Funders

Controls
|||
ALL TIME
JAN
FEB
MAR
APR
MAY
JUN
JUL
AUG
SEP
OCT
article

Contrasting Magnetic Structures in the Quaternary Sulfides Ba2FeMS5 (M = Sb, Bi)

Stanislav N. Savvin, Bradley C. Sheath, Simon J. Clarke
1 citations
Inorganic Chemistry
Magnetic and transport properties of perovskites and related materials
0.12
article

Contrasting Magnetic Structures in the Quaternary Sulfides Ba2FeMS5 (M = Sb, Bi)

Stanislav N. Savvin, Bradley C. Sheath, Simon J. Clarke
article en
1 citations

Abstract

Ba<sub>2</sub>FeSbS<sub>5</sub> and Ba<sub>2</sub>FeBiS<sub>5</sub> are two isostructural quaternary sulfides that crystallize in the <i>Pnma</i> space group with four formula units per unit cell. Ba<sub>2</sub>FeSbS<sub>5</sub> has lattice parameters <i>a</i> = 12.08609(3) Å, <i>b</i> = 8.83426(2) Å, and <i>c</i> = 8.89114(2) Å, and Ba<sub>2</sub>FeBiS<sub>5</sub> has <i>a</i> = 12.09610(3) Å, <i>b</i> = 8.89281(2) Å, and <i>c</i> = 8.82437(2) Å at room temperature. They comprise infinite [FeMS<sub>5</sub>]<sup>4-</sup> (M = Sb, Bi) chains, where Fe<sup>3+</sup> is present in FeS<sub>4</sub> tetrahedra and M<sup>3+</sup> ions reside in edge-sharing MS<sub>6</sub> distorted octahedra, each of which shares an edge with an FeS<sub>4</sub> tetrahedron. Powder neutron diffraction measurements confirm the presence of long-range antiferromagnetic order of the Fe<sup>3+</sup> moments in both materials, where Fe-S···S-Fe super-superexchange interactions which act along the direction of the [FeMS<sub>5</sub>]<sup>4-</sup> (M = Sb, Bi) chains are the driving force for this antiferromagnetic order. The magnetic Bragg reflections reside on a <i>k</i>-vector with <i>k</i> = (1/2 0 1/2), and the relative orientations of the moments are similar in the two cases One significant difference is that the moments are aligned along the crystallographic <i>b</i>-axis in Ba<sub>2</sub>FeSbS<sub>5</sub>, whereas in Ba<sub>2</sub>FeBiS<sub>5</sub> they lie along the longer crystallographic <i>a</i>-axis, reflecting the weak directional preference of the Fe<sup>3+</sup> moments. Furthermore, an additional incommensurately modulated ordering of the Fe<sup>3+</sup> moments is suggested for Ba<sub>2</sub>FeSbS<sub>5</sub> (but not Ba<sub>2</sub>FeBiS<sub>5</sub>) by the appearance of small additional magnetic Bragg peaks in the neutron diffraction data, which may be a consequence of greater magnetic frustration in Ba<sub>2</sub>FeSbS<sub>5</sub>.

Inorganic ChemistryVol. 63(49)
Universidad de Zaragoza (ES), University of Oxford (GB), Institut Laue-Langevin (FR), Instituto de Nanociencia y Materiales de Aragón (ES)
Diamond Light Source, Engineering and Physical Sciences Research Council
Openalex Percentile: Top 64%
Magnetic and transport properties of perovskites and related materials
0.12
AI Navigator

Ask Laika to Summarize, Analyze, and Connect papers live on the map.

Summarize Papers & Methodologies

Extract key findings, datasets, and comparative methods across publications.

Benchmark Rankings & Visual Analytics

Rank top research institutions, authors, funders, topics, and journals by Field-Weighted Citation Impact (FWCI) and paper volume with instant charts.

Connect Distant Disciplines

Bridge topological clusters on the map to find hidden collaborative intersections.