The ion conducting properties of perovskite solid solutions (La1/2Li1/3+X)TiO3

2005 ◽  
Vol 2 (1) ◽  
pp. 192-195 ◽  
Author(s):  
E. A. Fortalnova ◽  
A. V. Mosunov ◽  
M. G. Safronenko ◽  
N. U. Venskovskii ◽  
and E. D. Politova
ChemInform ◽  
2010 ◽  
Vol 33 (15) ◽  
pp. no-no
Author(s):  
Nobuhito Imanaka ◽  
Joachim Koehler ◽  
Shinji Tamura ◽  
Gin-ya Adachi

2006 ◽  
Vol 514-516 ◽  
pp. 407-411 ◽  
Author(s):  
Elena A. Fortalnova ◽  
Alexander V. Mosunov ◽  
Marina G. Safronenko ◽  
Nikolay U. Venskovskii ◽  
Ekaterina D. Politova

The influence of B-site substitution on electroconducting properties of perovskite-type solid solutions (La0.5Li0.5)[Ti1-x(M0.5Nb0.5)x]O3 with M = Al, Ga, have been studied. A decrease in the conductivity due to the unit cell contraction with increasing x in case of M = Al has been revealed. In case of Ga and Nb substitutions for Ti the unit cell volume has been found to increase with increasing x while the conductivity decreases due to the impurity phases presence. The high and low temperature anomalies on the temperature dependences of dielectric characteristic related to both the relaxation effect and phase transitions have been revealed.


2006 ◽  
Vol 42 (7) ◽  
pp. 806-814 ◽  
Author(s):  
E. D. Politova ◽  
B. A. Loginov ◽  
G. M. Kaleva ◽  
A. V. Mosunov ◽  
S. G. Prutchenko

2015 ◽  
Vol 8 (10) ◽  
pp. 2935-2940 ◽  
Author(s):  
David S. Mebane ◽  
Roger A. De Souza

The standard Poisson–Boltzmann approach to modeling the near-interface defect behaviour in solid electrolytes performs well at low dopant concentrations but its applicability is questionable at higher dopant levels where interactions become important.


1998 ◽  
Vol 547 ◽  
Author(s):  
Esther M. Ku ◽  
Evangeline M.E. Yeo ◽  
Bernhardt J. Wuensch

AbstractPyrochlore oxides, A2B2O7, are of interest as fuel cell materials and sensors because, with suitable doping, they may be fast-ion conducting or p- or n-type electronic conductors. An earlier analysis of Y2(ZryTi1-y)2O7 solid solutions showed that substitution of the larger Zr ion for Ti induced progressive disorder in both the cation and anion arrays causing a 103 increase in oxygen ion conductivity. In contrast, Y2(SnyTi1-y)2O7 solid solutions remained essentially fully ordered over their entire range of composition even though the range of average radii of the cation species in the B site overlapped to a considerable degree with those of the (ZryTi1-y) materials. The present work used Rietveld analysis of both neutron and x-ray powder profiles to examine Y2(ZrySn1-y)2O7 compositions along the third leg of the pseudo-ternary system: solid solutions between the stannate, with strong tendency to remain ordered, and the zirconate which has predilection toward complete disorder. Progressive disorder in the oxygen ion array was again observed with increasing y. Mixing between cation sites was found to progress at a rate independent of anion disordering. The behavior was very similar to Y2(ZryTi1-y)2O7, suggesting that the differing behavior of the three systems is due to the ability of Zr to readily enter the eight-coordinated A site.


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