Spin 1/2 Delafossite Honeycomb Compound Cu5SbO6

Cu5SbO6 is found to have a monoclinic, Delafossite-derived structure consisting of alternating layers of O–Cu­(I)–O sticks and magnetic layers of Jahn–Teller distorted Cu­(II)­O6 octahedra in an edge sharing honeycomb arrangement with Sb­(V)­O6 octahedra. This yields the structural formula Cu­(I)3Cu...

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Veröffentlicht in:Inorganic chemistry 2012-01, Vol.51 (1), p.557-565
Hauptverfasser: Climent-Pascual, E, Norby, P, Andersen, N.H, Stephens, P.W, Zandbergen, H.W, Larsen, J, Cava, R.J
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container_end_page 565
container_issue 1
container_start_page 557
container_title Inorganic chemistry
container_volume 51
creator Climent-Pascual, E
Norby, P
Andersen, N.H
Stephens, P.W
Zandbergen, H.W
Larsen, J
Cava, R.J
description Cu5SbO6 is found to have a monoclinic, Delafossite-derived structure consisting of alternating layers of O–Cu­(I)–O sticks and magnetic layers of Jahn–Teller distorted Cu­(II)­O6 octahedra in an edge sharing honeycomb arrangement with Sb­(V)­O6 octahedra. This yields the structural formula Cu­(I)3Cu­(II)2Sb­(V)­O6. Variants with ordered and disordered layer stacking are observed, depending on the synthesis conditions. The spin 1/2 Cu2+ ions form dimers in the honeycomb layer. The magnetic susceptibility measured between 5 and 300 K is characteristic of the presence of a singlet–triplet spin gap of 189 K. High resolution synchrotron X-ray diffraction studies indicate that changes in the intra- or interdimer distances between 300 and 20 K, such as might indicate an increase in strength of the Peierls-like distortion through the spin gap temperature, if present, are very small. A comparison to the NaFeO2-type Cu2+ honeycomb compounds Na3Cu2SbO6 and Na2Cu2TeO6 is presented.
doi_str_mv 10.1021/ic202066n
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This yields the structural formula Cu­(I)3Cu­(II)2Sb­(V)­O6. Variants with ordered and disordered layer stacking are observed, depending on the synthesis conditions. The spin 1/2 Cu2+ ions form dimers in the honeycomb layer. The magnetic susceptibility measured between 5 and 300 K is characteristic of the presence of a singlet–triplet spin gap of 189 K. High resolution synchrotron X-ray diffraction studies indicate that changes in the intra- or interdimer distances between 300 and 20 K, such as might indicate an increase in strength of the Peierls-like distortion through the spin gap temperature, if present, are very small. 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