{110}-Layered B-cation ordering in the anion-deficient perovskite Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 with the crystallographic shear structure

A novel anion-deficient perovskite-based compound, Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 , was synthesized via the citrate-based route. This compound is an n = 5 member of the A n B n O 3n−2 homologous series with unit-cell parameters related to the perovskite subcell a p ≈ 4.0 Å as a p √2 × a p × 5 a p √2...

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Veröffentlicht in:Dalton transactions : an international journal of inorganic chemistry 2015, Vol.44 (23), p.10753-10762
Hauptverfasser: Tyablikov, O. A., Batuk, D., Tsirlin, A. A., Batuk, M., Verchenko, V. Yu, Filimonov, D. S., Pokholok, K. V., Sheptyakov, D. V., Rozova, M. G., Hadermann, J., Antipov, E. V., Abakumov, A. M.
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container_title Dalton transactions : an international journal of inorganic chemistry
container_volume 44
creator Tyablikov, O. A.
Batuk, D.
Tsirlin, A. A.
Batuk, M.
Verchenko, V. Yu
Filimonov, D. S.
Pokholok, K. V.
Sheptyakov, D. V.
Rozova, M. G.
Hadermann, J.
Antipov, E. V.
Abakumov, A. M.
description A novel anion-deficient perovskite-based compound, Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 , was synthesized via the citrate-based route. This compound is an n = 5 member of the A n B n O 3n−2 homologous series with unit-cell parameters related to the perovskite subcell a p ≈ 4.0 Å as a p √2 × a p × 5 a p √2. The crystal structure of Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 consists of quasi-2D perovskite blocks with a thickness of three octahedral layers separated by the 1/2[110](1̄01) p crystallographic shear (CS) planes, which are parallel to the {110} plane of the perovskite subcell. The CS planes transform the corner-sharing octahedra into chains of edge-sharing distorted tetragonal pyramids. Using a combination of neutron powder diffraction, 57 Fe Mössbauer spectroscopy and atomic resolution electron energy-loss spectroscopy we demonstrate that the B-cations in Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 are ordered along the {110} perovskite layers with Fe 3+ in distorted tetragonal pyramids along the CS planes, Ti 4+ preferentially in the central octahedra of the perovskite blocks and Sc 3+ in the outer octahedra of the perovskite blocks. Magnetic susceptibility and Mössbauer spectroscopy indicate a broadened magnetic transition around T N ∼ 45 K and the onset of local magnetic fields at low temperatures. The magnetic order is probably reminiscent of that in other A n B n O 3n−2 homologues, where G-type AFM order within the perovskite blocks has been observed.
doi_str_mv 10.1039/C4DT03867C
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The crystal structure of Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 consists of quasi-2D perovskite blocks with a thickness of three octahedral layers separated by the 1/2[110](1̄01) p crystallographic shear (CS) planes, which are parallel to the {110} plane of the perovskite subcell. The CS planes transform the corner-sharing octahedra into chains of edge-sharing distorted tetragonal pyramids. Using a combination of neutron powder diffraction, 57 Fe Mössbauer spectroscopy and atomic resolution electron energy-loss spectroscopy we demonstrate that the B-cations in Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 are ordered along the {110} perovskite layers with Fe 3+ in distorted tetragonal pyramids along the CS planes, Ti 4+ preferentially in the central octahedra of the perovskite blocks and Sc 3+ in the outer octahedra of the perovskite blocks. 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Magnetic susceptibility and Mössbauer spectroscopy indicate a broadened magnetic transition around T N ∼ 45 K and the onset of local magnetic fields at low temperatures. The magnetic order is probably reminiscent of that in other A n B n O 3n−2 homologues, where G-type AFM order within the perovskite blocks has been observed.</abstract><doi>10.1039/C4DT03867C</doi><tpages>10</tpages></addata></record>
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title {110}-Layered B-cation ordering in the anion-deficient perovskite Pb 2.4 Ba 2.6 Fe 2 Sc 2 TiO 13 with the crystallographic shear structure
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