Hostname: page-component-848d4c4894-tn8tq Total loading time: 0 Render date: 2024-06-20T13:32:29.848Z Has data issue: false hasContentIssue false

Bi2Sr2M'2M”O11.5 [(M' = Nb, Ta) and (M” = Al, Ga)], Synthesis and Characterization of Oxygen-Deficient Aurivillius Phases

Published online by Cambridge University Press:  16 February 2011

Kurt R. Kendall
Affiliation:
Department of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139
Carlos J. Navas
Affiliation:
Department of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139
Hans-Conrad Zur Loye
Affiliation:
Department of Chemistry, Massachusetts Institute of Technology, Cambridge, MA 02139
Get access

Abstract

Oxygen-deficient layered bismuth oxides, Bi2Sr2M'2M”O11.5 [(M' = Nb, Ta) and (M” = Al, Ga)] were synthesized. Powder X-ray diffraction and transmission electron microscopy were usedto characterize the new materials' structures. The ionic conductivity was measuredusing impedance spectroscopy which indicated the existence of multiple conductive states in the new oxygen-deficient materials. Arrhenius plots of the conductivity showed discontinuities which were attributed to transitions between different conductive states. At 800ºC, Bi2Sr2Nb2GaO11.5 and Bi2Sr2Nb2A1O1.5, have ionic conductivities of 2.0×10−2 S/cm and 1.2×10−2 S/cm, respectively. Differential thermal analysis showed phase transitions in the oxygen-deficient materials. These transitionsoccurred at temperatures similar to those at which discontinuities were observed in the Arrhenius plots of the conductivity and are attributed to oxygen vacancy order/disorder transitions. The transference number was calculated for some of the samples by measuring both the EMF and the conductivity as a function of oxygen partial pressure. Under atmospheric conditions the new materials are predominantly ionic conductors.

Type
Research Article
Copyright
Copyright © Materials Research Society 1995

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

1. Minh, N. Q., J. Am. Ceram. Soc. 76, 563 (1993).Google Scholar
2. Cosimo, R. Di, Burrington, J. D., Grasselli, R. K., J. Catal. 102, 234 (1986).Google Scholar
3. Hagenmuller, P., in Superionic Solids and Solid Electrolytes Laskar, A. L., Chandra, S., Eds. (Academic Press, New York, 1989) p. 679.Google Scholar
4. Riess, I., in Science and Technology of Fast Ion Conductors Tuller, H. L., Balkanski, M., Eds. (Plenum Press, New York, 1987) p. 23.Google Scholar
5. Kudo, T., Fueki, K., Solid State Ionics (VCH Publishers, New York, 1990)Google Scholar
6. Takahashi, T., Iwahara, H., Esaka, T., J. Electrochem. Soc. 124, 1563 (1977).Google Scholar
7. Steele, B. C. H., J. Power Sources 49, 1 (1994).Google Scholar
8. Aurivillius, B., Arkiv. Kemi. 1, 463 (1949).Google Scholar
9. Kendall, K. R., Thomas, J. K., Loye, H. C. zur, Chem. Mater., In Press (1994).Google Scholar
10. Kendall, K. R., Thomas, J. K., zur Loye, H.-C., Solid State Ionics 70/71, 221 (1994).Google Scholar
11. Fendorf, M., U.C. Berkeley, Portions of the TEM work were performed at the National Center for Electron Microscopy, Lawrence Berkeley Laboratory, a facility funded by the Director, Office of Energy Research, Office of Basic Energy Sciences, Materials Science Division of the U.S. Department of Energy under Contract Number DE-AC03-76SF00098 (1994).Google Scholar
12. Subbarao, E. C., J. Am. Ceram. Soc. 45, 166 (1962).Google Scholar
13. Tuller, H. L., Moon, P. K., Mater. Sci. Eng. B-Solid State M. B1, 171 (1988).Google Scholar