Journal
CRYSTENGCOMM
Volume 23, Issue 47, Pages 8404-8410Publisher
ROYAL SOC CHEMISTRY
DOI: 10.1039/d1ce00990g
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Funding
- Ministry of Education, Culture, Sports, Science and Technology of Japan [15H02021]
- Grants-in-Aid for Scientific Research [15H02021] Funding Source: KAKEN
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The phase stability of Aurivillius bismuth-layer structured Bi5Ti3FeO15 (BTFO15) was investigated in an epitaxial pillar-matrix nanocomposite system with spinel ferrites. Different super periodic structures of BTFOs appeared depending on the growth temperature, denoted by BTFO15 center dot nBiFeO(3) with continuous values of n between -0.5 and +1. The formation mechanism of such structures was discussed in terms of the ordering of Bi2O22+ layers in perovskite blocks, driven by Fe3+ transfer between BTFO15 and spinel ferrites during phase separation.
The phase stability of Aurivillius bismuth-layer structured Bi5Ti3FeO15 (BTFO15) has been investigated in an epitaxial pillar-matrix nanocomposite system with spinel ferrites. Depending on the growth temperature a variety of super periodic structures of BTFOs appeared, denoted by the general formula BTFO15 center dot nBiFeO(3) with almost continuous values of n between -0.5 and +1. In nanocomposites with CFO, n takes the positive values from n = 0, increasing up to n = 1 corresponding to Bi6Ti3Fe2O18 (BTFO18), as the growth temperature decreases. In contrast, in nanocomposites with NFO, n takes the negative values from n = 0, decreasing close to -0.5 corresponding to a well-known intergrowth structure of Bi4Ti3O12 (BIT)-BTFO15, as the growth temperature increases. The formation mechanism of such super periodic structures is discussed in terms of the ordering of Bi2O22+ layers in the perovskite blocks, driven by the Fe3+ transfer between BTFO15 and spinel ferrites as starting materials during phase separation, depending on the degree of excess or deficiency of the Bi amount.
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