Magnetism and 3D Electron Diffraction Solution of Hydrated Rubidium–Ruthenium Oxide Rb <sub>2</sub> Ru <sub>2</sub> O <sub>7</sub> ·H <sub>2</sub> O

The crystal structure of Rb<sub>2</sub>Ru<sub>2</sub>O<sub>7</sub>·H<sub>2</sub>O was determined by three-dimensional electron diffraction from the individual crystallites of a solid-state powder product. Rb<sub>2</sub>Ru<sub>2</sub>O<sub>7</sub>·H<sub>2</sub>O crystallizes in space group <i>C</i>2/<i>c</i> (<i>a</i> = 7.841(3) Å, <i>b</i> = 12.500(3) Å, <i>c</i> = 8.392(2) Å, β = 93.57(4)°, Z = 4). The structure contains infinite chains that run normal to the (101) plane and consist of alternating RuO<sub>6</sub> octahedra and square-pyramidal RuO<sub>5</sub> units connected via shared O-O edges. Magnetic properties were measured on the bulk powder, showing a diamagnetic baseline from 300 K to 60 K with a small Curie tail below 55 K. The magnetic moment, calculated from the 1.8 K isotherm, saturates at <i>M</i> = 4.4 × 10<sup>-3</sup> μ<sub>B</sub> Ru<sup>-1</sup>, much less than would be expected for <i>S</i> = 1 ruthenium. Bond-valence-sum analysis indicates high-valent Ru, and the near-diamagnetic response is consistent with the edge-sharing Ru-Ru motif, where weak direct Ru-Ru overlap yields a local singlet.

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Journal
Inorganic Chemistry
Published
2026-02-18
DOI
https://doi.org/10.1021/acs.inorgchem.6c00345
Primary Topic
Magnetism in coordination complexes
Type
article
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article

Magnetism and 3D Electron Diffraction Solution of Hydrated Rubidium–Ruthenium Oxide Rb 2 Ru 2 O 7 ·H 2 O

C. BELL, Simon R. Hall, Krystof Chrappova, Jeremiah P. Tidey
Inorganic Chemistry
Magnetism in coordination complexes
article

Magnetism and 3D Electron Diffraction Solution of Hydrated Rubidium–Ruthenium Oxide Rb 2 Ru 2 O 7 ·H 2 O

C. BELL, Simon R. Hall, Krystof Chrappova, Jeremiah P. Tidey
article en

Abstract

The crystal structure of Rb<sub>2</sub>Ru<sub>2</sub>O<sub>7</sub>·H<sub>2</sub>O was determined by three-dimensional electron diffraction from the individual crystallites of a solid-state powder product. Rb<sub>2</sub>Ru<sub>2</sub>O<sub>7</sub>·H<sub>2</sub>O crystallizes in space group <i>C</i>2/<i>c</i> (<i>a</i> = 7.841(3) Å, <i>b</i> = 12.500(3) Å, <i>c</i> = 8.392(2) Å, β = 93.57(4)°, Z = 4). The structure contains infinite chains that run normal to the (101) plane and consist of alternating RuO<sub>6</sub> octahedra and square-pyramidal RuO<sub>5</sub> units connected via shared O-O edges. Magnetic properties were measured on the bulk powder, showing a diamagnetic baseline from 300 K to 60 K with a small Curie tail below 55 K. The magnetic moment, calculated from the 1.8 K isotherm, saturates at <i>M</i> = 4.4 × 10<sup>-3</sup> μ<sub>B</sub> Ru<sup>-1</sup>, much less than would be expected for <i>S</i> = 1 ruthenium. Bond-valence-sum analysis indicates high-valent Ru, and the near-diamagnetic response is consistent with the edge-sharing Ru-Ru motif, where weak direct Ru-Ru overlap yields a local singlet.

Inorganic ChemistryVol. 65(8)
University of Bristol (GB), University of Warwick (GB)
Openalex Percentile: Top 53%
Magnetism in coordination complexes
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