Crystal structure and spin-trimer magnetism of Rb 2.3 (H 2 O) 0.8 Mn 3 [B 4 P 6 O 24 (O,OH) 2 ]
The novel borophosphate Rb (H O) Mn [B P O (O,OH) ] was prepared under hydrothermal conditions at 553 K. Its crystal structure was determined using single-crystal X-ray diffraction data obtained from a non-merohedral twin and refined against F to R = 0.057. The compound crystallizes in the orthorhom...
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Veröffentlicht in: | Dalton transactions : an international journal of inorganic chemistry 2017-02, Vol.46 (9), p.2957-2965 |
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Hauptverfasser: | , , , , , , , , , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The novel borophosphate Rb
(H
O)
Mn
[B
P
O
(O,OH)
] was prepared under hydrothermal conditions at 553 K. Its crystal structure was determined using single-crystal X-ray diffraction data obtained from a non-merohedral twin and refined against F
to R = 0.057. The compound crystallizes in the orthorhombic space group Pbcn, with unit-cell parameters a = 20.076(2) Å, b = 9.151(1) Å, c = 12.257(1) Å, V = 2251.8(2) Å
, and Z = 4. The title compound is the first example of a borophosphate with manganese ions adopting both octahedral and tetrahedral coordinations. Its unique crystal structure is formed by borophosphate slabs and chains of Mn
-centered polyhedra sharing edges and vertices. These 2D and 1D fragments interconnect into a framework with open channels that accommodate Rb
cations and water molecules. Topological relationships between borophosphates built from three-membered rings of two borate and one phosphate tetrahedra sharing oxygen vertices, amended by additional PO
and HPO
tetrahedra, are discussed. The temperature dependence of the magnetic susceptibility of Rb
(H
O)
Mn
[B
P
O
(O,OH)
] reveals predominant antiferromagnetic exchange interactions and the high-temperature effective magnetic moment corresponding to the high-spin S = 5/2 state of Mn
ions. At 12.5 K, a magnetic transition is evidenced by ac-susceptibility and specific heat measurements. A spin-trimer model with the leading exchange interaction J ∼ 3.2 K is derived from density-functional band-structure calculations and accounts for all experimental observations. |
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ISSN: | 1477-9226 1477-9234 |
DOI: | 10.1039/C6DT04241D |