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Temperature Dependence of Ion Irradiation Induced Amorphization of Zirconolite

Published online by Cambridge University Press:  10 February 2011

K.L. Smith
Affiliation:
Materials Division, Australian Nuclear Science and Technology Organisation, P.M.B. 1, Menai, NSW 2234, AUSTRALIA
M.G. Blackford
Affiliation:
Materials Division, Australian Nuclear Science and Technology Organisation, P.M.B. 1, Menai, NSW 2234, AUSTRALIA
G.R. Lumpkin
Affiliation:
Materials Division, Australian Nuclear Science and Technology Organisation, P.M.B. 1, Menai, NSW 2234, AUSTRALIA
N.J. Zaluzec
Affiliation:
Materials Science Division, Argonne National Laboratory, 9700 South Cass Ave, Argonne, II 60439, USA
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Abstract

The critical dose for amorphisation, Dc, of two end-member zirconolites (CaZrTi2O7) with different stacking fault densities, was measured as a function of irradiation temperature from 20 K to 623 K using the HVEM-Tandem Facility at Argonne National Laboratory (ANL). Below 473 K, the Dc, values of both samples are identical within experimental error, showing only a small increase in Dc, from (2.5 to 4.6) × 1018 ions m−2 between 20 K and 473 K. At temperatures above 473 K, the data for the zirconolite containing many stacking faults is bracketed by two data sets from almost crystallographically perfect end-member zirconolites: one collected in this study and one collected in a previous study. The raw Dc versus temperature data from the zirconolites in this and a previous study suggest that the critical temperature above which samples cannot be amorphised and/or recrystallisation is complete, Tc, is between 600 and 1000 K. The data sets collected in this study are discussed in relation to a current model.

Type
Research Article
Copyright
Copyright © Materials Research Society 2000

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References

REFERENCES

[1] Ewing, R.C., Weber, W.J. and Clinard, F.W. Jr, Progress in Nuclear Energy, 29 [2], 63127 (1995).Google Scholar
[2] Lumpkin, G.R., Smith, K.L., Blackford, M.G. Giere, R. and Williams, C.T., Mat. Res. Soc. Symp. Proc., 506, 215222 (1998).Google Scholar
[3] Jostsons, A., Vance, E.R. and Ebbingaus, B. (1999) Immobilisation of surplus plutonium in titanate ceramics, presented at Global'99 “Nuclear Technology - Bridging the Millenia”, Jackson Hole, Wyoming, USA, Aug. 29 - Sept. 3 1999.Google Scholar
[4] Vance, E.R., Ball, C.J., Blackford, M.G., Cassidy, D.J. and Smith, K.L., J. Nucl. Mater., 175, p.5866 (1990).Google Scholar
[5] Gupta, P.K., J. Am. Ceram. Soc., 76(5), 10881095 (1993).Google Scholar
[6] Hobbs, L.W., Seeram, A.N., Jesurum, C.E. and Berger, B.A., Nucl. Instruments and Meths. in Phys Res., B116, 1825 (1996).Google Scholar
[7] Wang, S.X., Wang, L.M. and Ewing, R.C., Nuc. Instruments and Meths. in Phys. Res., B127/128, 186190 (1997).Google Scholar
[8] Weber, W.J., Ewing, R.C. and Wang, L.M., J. Mater. Res., 9(3), 688698 (1994).Google Scholar
[9] Ringwood, A.E., Kesson, S.E., Reeve, K.D., Levins, D.M. and Ramm, E.J. (1988) Synroc, in Radioactive Waste Forms for the Future, edited by Lutze, W. and Ewing, R.C., Elsevier, p.233334.Google Scholar
[10] Smith, K.L., Lumpkin, G.R. and Zaluzec, N.J., J. Nucl. Materials, 250, 3652 (1997).Google Scholar
[11] Wang, S.X., Lumpkin, G.R., Wang, L.M. and Ewing, R.C., in Radiation Effects in Insulators, REI-10, July 18-23, 1999, Jena, Germany (1999).Google Scholar
[12] White, T. J., Mitamura, H., Hojou, K. and Furuno, S., Mat. Res. Soc. Symp. Proc. Vol. 333, 227232 (1994).Google Scholar
[13] Clinard, F.W. Jr, Am. Ceram. Soc. Bull., 65, 1181–87 (1986).Google Scholar
[14] Meldrum, A., Zinkle, S.J., Boatner, L.A. and Ewing, R.C., Phys Rev. B, 59(6) 39813992 (1999)Google Scholar