Magnetic Structures and Magnetic Phase Diagram of the Mixed-Valence Iron Phosphate Fe <sub>7</sub> (PO <sub>4</sub> ) <sub>6</sub>

Mixed-valence iron compounds are fascinating materials exemplified by ferrimagnetic Fe<sub>3</sub>O<sub>4</sub>, multiferroic LuFe<sub>2</sub>O<sub>4</sub>, and a pigment Fe<sub>4</sub>[Fe(CN)<sub>6</sub>]<sub>3</sub>. Mixed-valent iron (oxy)phosphates also provide a large variety of different connections between magnetic ions, which are responsible for complex magnetism. Fe<sub>7</sub>(PO<sub>4</sub>)<sub>6</sub> (Fe<sub>3</sub><sup>2+</sup>Fe<sub>4</sub><sup>3+</sup>(PO<sub>4</sub>)<sub>6</sub>) has well-defined Fe<sup>2+</sup> and Fe<sup>3+</sup> sites and shows two antiferromagnetic transitions at <i>T</i><sub>N1</sub> = 47 K and <i>T</i><sub>N2</sub> = 16 K. Here, we investigated magnetic structures of Fe<sub>7</sub>(PO<sub>4</sub>)<sub>6</sub> (at zero magnetic field) using neutron powder diffraction and constructed a temperature-magnetic-field phase diagram. Below <i>T</i><sub>N1</sub>, magnetic propagation vector is <b><i>k</i></b><sub><b>1</b></sub> = (1/2, 0, 1/2), and magnetic moments on Fe<sup>3+</sup> sites are nearly fully ordered; while moments on Fe<sup>2+</sup> sites are significantly reduced. Below <i>T</i><sub>N2</sub>, the second propagation vector appears <b><i>k</i></b><sub><b>2</b></sub> = (0, 1/2, 0) and coexists with <b><i>k</i></b><sub><b>1</b></sub>; moments on Fe<sup>2+</sup> sites are fully ordered (at 2 K) reaching 4.5 μ<sub>B</sub> suggesting noticeable spin-orbital contributions. Coexistence of two propagation vectors and triclinic symmetry results in variations of total magnetic moments on each site. Magnetic measurements up to 300 kOe detected one field-induced transition near 55.5 kOe. Data showed that <i>T</i><sub>N1</sub> is nearly magnetic-field independent up to 90 kOe, while a more complex behavior was observed near <i>T</i><sub>N2</sub> at magnetic fields around 50 kOe.

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Journal
Inorganic Chemistry
Published
2026-03-26
DOI
https://doi.org/10.1021/acs.inorgchem.6c00534
Primary Topic
Crystal Structures and Properties
Type
article
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article

Magnetic Structures and Magnetic Phase Diagram of the Mixed-Valence Iron Phosphate Fe 7 (PO 4 ) 6

Andreas Dönni, Naohito Tsujii, Alexei Belik, Vladimir Y. Pomjakushin et al.
Inorganic Chemistry
Crystal Structures and Properties
article

Magnetic Structures and Magnetic Phase Diagram of the Mixed-Valence Iron Phosphate Fe 7 (PO 4 ) 6

Andreas Dönni, Naohito Tsujii, Alexei Belik, Vladimir Y. Pomjakushin, Lukas Keller
article en

Abstract

Mixed-valence iron compounds are fascinating materials exemplified by ferrimagnetic Fe<sub>3</sub>O<sub>4</sub>, multiferroic LuFe<sub>2</sub>O<sub>4</sub>, and a pigment Fe<sub>4</sub>[Fe(CN)<sub>6</sub>]<sub>3</sub>. Mixed-valent iron (oxy)phosphates also provide a large variety of different connections between magnetic ions, which are responsible for complex magnetism. Fe<sub>7</sub>(PO<sub>4</sub>)<sub>6</sub> (Fe<sub>3</sub><sup>2+</sup>Fe<sub>4</sub><sup>3+</sup>(PO<sub>4</sub>)<sub>6</sub>) has well-defined Fe<sup>2+</sup> and Fe<sup>3+</sup> sites and shows two antiferromagnetic transitions at <i>T</i><sub>N1</sub> = 47 K and <i>T</i><sub>N2</sub> = 16 K. Here, we investigated magnetic structures of Fe<sub>7</sub>(PO<sub>4</sub>)<sub>6</sub> (at zero magnetic field) using neutron powder diffraction and constructed a temperature-magnetic-field phase diagram. Below <i>T</i><sub>N1</sub>, magnetic propagation vector is <b><i>k</i></b><sub><b>1</b></sub> = (1/2, 0, 1/2), and magnetic moments on Fe<sup>3+</sup> sites are nearly fully ordered; while moments on Fe<sup>2+</sup> sites are significantly reduced. Below <i>T</i><sub>N2</sub>, the second propagation vector appears <b><i>k</i></b><sub><b>2</b></sub> = (0, 1/2, 0) and coexists with <b><i>k</i></b><sub><b>1</b></sub>; moments on Fe<sup>2+</sup> sites are fully ordered (at 2 K) reaching 4.5 μ<sub>B</sub> suggesting noticeable spin-orbital contributions. Coexistence of two propagation vectors and triclinic symmetry results in variations of total magnetic moments on each site. Magnetic measurements up to 300 kOe detected one field-induced transition near 55.5 kOe. Data showed that <i>T</i><sub>N1</sub> is nearly magnetic-field independent up to 90 kOe, while a more complex behavior was observed near <i>T</i><sub>N2</sub> at magnetic fields around 50 kOe.

Inorganic Chemistry
National Institute for Materials Science (JP)
Openalex Percentile: Top 9%
Crystal Structures and Properties
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