TY - JOUR
T1 - Suppression of intersite charge transfer in charge-disproportionated perovskite YCu3Fe4O12
AU - Etani, Hidenobu
AU - Yamada, Ikuya
AU - Ohgushi, Kenya
AU - Hayashi, Naoaki
AU - Kusano, Yoshihiro
AU - Mizumaki, Masaichiro
AU - Kim, Jungeun
AU - Tsuji, Naruki
AU - Takahashi, Ryoji
AU - Nishiyama, Norimasa
AU - Inoue, Toru
AU - Irifune, Tetsuo
AU - Takano, Mikio
PY - 2013/4/24
Y1 - 2013/4/24
N2 - A novel iron perovskite YCu3Fe4O12 was synthesized under high pressure and high temperature of 15 GPa and 1273 K. Synchrotron X-ray and electron diffraction measurements have demonstrated that this compound crystallizes in the cubic AA′3B4O 12-type perovskite structure (space group Im3Ì..., No. 204) with a lattice constant of a = 7.30764(10) Å at room temperature. YCu 3Fe4O12 exhibits a charge disproportionation of 8Fe3.75+ → 3Fe5+ + 5Fe3+, a ferrimagnetic ordering, and a metal-semiconductor-like transition simultaneously at 250 K, unlike the known isoelectronic compound LaCu3Fe4O 12 that currently shows an intersite charge transfer of 3Cu 2+ + 4Fe3.75+ → 3Cu3+ + 4Fe3+, an antiferromagnetic ordering, and a metal-insulator transition at 393 K. This finding suggests that intersite charge transfer is not the only way of relieving the instability of the Fe3.75+ state in the A3+Cu 2+3Fe3.75+4O12 perovskites. Crystal structure analysis reveals that bond strain, rather than the charge account of the A-site alone, which is enhanced by large A 3+ ions, play an important role in determining which of intersite charge transfer or charge disproportionation is practical.
AB - A novel iron perovskite YCu3Fe4O12 was synthesized under high pressure and high temperature of 15 GPa and 1273 K. Synchrotron X-ray and electron diffraction measurements have demonstrated that this compound crystallizes in the cubic AA′3B4O 12-type perovskite structure (space group Im3Ì..., No. 204) with a lattice constant of a = 7.30764(10) Å at room temperature. YCu 3Fe4O12 exhibits a charge disproportionation of 8Fe3.75+ → 3Fe5+ + 5Fe3+, a ferrimagnetic ordering, and a metal-semiconductor-like transition simultaneously at 250 K, unlike the known isoelectronic compound LaCu3Fe4O 12 that currently shows an intersite charge transfer of 3Cu 2+ + 4Fe3.75+ → 3Cu3+ + 4Fe3+, an antiferromagnetic ordering, and a metal-insulator transition at 393 K. This finding suggests that intersite charge transfer is not the only way of relieving the instability of the Fe3.75+ state in the A3+Cu 2+3Fe3.75+4O12 perovskites. Crystal structure analysis reveals that bond strain, rather than the charge account of the A-site alone, which is enhanced by large A 3+ ions, play an important role in determining which of intersite charge transfer or charge disproportionation is practical.
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U2 - 10.1021/ja312015j
DO - 10.1021/ja312015j
M3 - Article
C2 - 23560478
AN - SCOPUS:84876727410
SN - 0002-7863
VL - 135
SP - 6100
EP - 6106
JO - Journal of the American Chemical Society
JF - Journal of the American Chemical Society
IS - 16
ER -