TY - JOUR
T1 - Effect of Y2O3 addition on the conductivity and elastic modulus of (CeO2)1 - x(YO1.5)x
AU - Sato, Kazuhisa
AU - Suzuki, Ken
AU - Yashiro, Keiji
AU - Kawada, Tatsuya
AU - Yugami, Hiroo
AU - Hashida, Toshiyuki
AU - Atkinson, Alan
AU - Mizusaki, Junichiro
N1 - Funding Information:
This study was partly supported by a Grant-in-Aid for Scientific Research on Priority Area, “Nanoionics (439),” and Grant-in-Aid for Scientific Research (B) (No.18360053) from the MEXT.
PY - 2009/8/17
Y1 - 2009/8/17
N2 - The conductivity and elastic modulus of (CeO2)1 - x(YO1.5)x for x values of 0.10, 0.15, 0.20, 0.30, and 0.40 were investigated by experiments and molecular dynamics simulations. The calculated conductivity exhibited a maximum value at approximately 15 mol% Y2O3; this trend agreed with that of the experimental results. In order to clarify the reason for the occurrence of the maximum conductivity, the paths for the transfer of oxygen vacancies were counted. The numerical result revealed that as the content of Y2O3 dopant increases, the number of paths for the transfer of oxygen vacancies decreases, whereas the number of oxygen vacancies for conductivity increases. Thus, the trade-off between the increase in the number of vacancy sites and the decrease in the vacancy transfer was considered to be the reason for the maximum conductivity occurring at the Y2O3 dopant content of approximately 15 mol%. The calculated elastic modulus also exhibited a minimum value at approximately 20 mol% Y2O3, which also agreed with the experimental results. It was shown that the Y-O-Y bonding energy increased with the increasing content of Y2O3 dopant. Thus, the trade-off between the increase in the number of vacancy sites and that in the Y-O-Y bonding energy was considered to be the reason for the minimum elastic modulus occurring at the Y2O3 dopant content of approximately 20 mol%.
AB - The conductivity and elastic modulus of (CeO2)1 - x(YO1.5)x for x values of 0.10, 0.15, 0.20, 0.30, and 0.40 were investigated by experiments and molecular dynamics simulations. The calculated conductivity exhibited a maximum value at approximately 15 mol% Y2O3; this trend agreed with that of the experimental results. In order to clarify the reason for the occurrence of the maximum conductivity, the paths for the transfer of oxygen vacancies were counted. The numerical result revealed that as the content of Y2O3 dopant increases, the number of paths for the transfer of oxygen vacancies decreases, whereas the number of oxygen vacancies for conductivity increases. Thus, the trade-off between the increase in the number of vacancy sites and the decrease in the vacancy transfer was considered to be the reason for the maximum conductivity occurring at the Y2O3 dopant content of approximately 15 mol%. The calculated elastic modulus also exhibited a minimum value at approximately 20 mol% Y2O3, which also agreed with the experimental results. It was shown that the Y-O-Y bonding energy increased with the increasing content of Y2O3 dopant. Thus, the trade-off between the increase in the number of vacancy sites and that in the Y-O-Y bonding energy was considered to be the reason for the minimum elastic modulus occurring at the Y2O3 dopant content of approximately 20 mol%.
KW - (CeO)(YO)
KW - AC impedance method
KW - Conductivity
KW - Elastic modulus
KW - Molecular dynamics
KW - Small punch (SP) testing method
KW - Solid oxide fuel cell (SOFC)
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U2 - 10.1016/j.ssi.2009.06.003
DO - 10.1016/j.ssi.2009.06.003
M3 - Article
AN - SCOPUS:67651151034
SN - 0167-2738
VL - 180
SP - 1220
EP - 1225
JO - Solid State Ionics
JF - Solid State Ionics
IS - 20-22
ER -