TY - JOUR
T1 - Sequential variation of super periodic structures emerged in Bi-layered perovskite pillar-matrix epitaxial nanocomposite films with spinel ferrites
AU - Harada, R.
AU - Kawahira, Y.
AU - Ikeda, T.
AU - Maruyama, S.
AU - Matsumoto, Y.
N1 - Funding Information:
The authors would like to thank Prof. Kazuo Sasaki in Tohoku University for his helpful suggestions in discussing the Bi2O22+ layer ordering model. This work has been partially supported by a Grant-in-Aid for Scientific Research (No.15H02021) from the Ministry of Education, Culture, Sports, Science and Technology of Japan.
Publisher Copyright:
© The Royal Society of Chemistry.
PY - 2021/12/21
Y1 - 2021/12/21
N2 - 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·nBiFeO3 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.
AB - 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·nBiFeO3 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.
UR - http://www.scopus.com/inward/record.url?scp=85121027599&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85121027599&partnerID=8YFLogxK
U2 - 10.1039/d1ce00990g
DO - 10.1039/d1ce00990g
M3 - Article
AN - SCOPUS:85121027599
SN - 1466-8033
VL - 23
SP - 8404
EP - 8410
JO - CrystEngComm
JF - CrystEngComm
IS - 47
ER -