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Nanosized Thallium Inclusions in Aluminium

Published online by Cambridge University Press:  22 February 2011

E. Johnson
Affiliation:
Niels Bohr Institute for Astronomy, Physics and Geophysics, Ørsted Laboratory, Universitetsparken 5, DK-2100 Copenhagen Ø, Denmark
A. Johansen
Affiliation:
Niels Bohr Institute for Astronomy, Physics and Geophysics, Ørsted Laboratory, Universitetsparken 5, DK-2100 Copenhagen Ø, Denmark
H.H. Andersen
Affiliation:
Niels Bohr Institute for Astronomy, Physics and Geophysics, Ørsted Laboratory, Universitetsparken 5, DK-2100 Copenhagen Ø, Denmark
L. Sarholt-Kristensen
Affiliation:
Niels Bohr Institute for Astronomy, Physics and Geophysics, Ørsted Laboratory, Universitetsparken 5, DK-2100 Copenhagen Ø, Denmark
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Abstract

Ion implantation of pure aluminium with thallium induces formation of nanosized crystalline thallium inclusions with either fee or bee structure. The size of the inclusions depends on the implantation conditions and subsequent annealing treatments. Inclusions less than 10-15 nm in size are generally fee while larger inclusions are bee. The fee inclusions are aligned topotactically with the aluminium matrix with a cube/cube orientation relationship, and they have a truncated octahedral shape bounded by {111} and {001} planes. The lattice parameter of the fee thallium inclusions is 0.484 nm ± 0.002 nm, which is slightly but significantly larger than for the high pressure fee thallium phase known to be stable above 3.8 GPa. The lattice parameter of the bec inclusions is close to the equilibrium value of 0.387 nm and the orientation relationship is given by the Kurdjumov-Sachs rule (011)bcc ║ (111)fcc and [111]bcc ║ [101]fcc The bec inclusions,, representing the high temperature equilibrium phase but existing in metastable equilibrium at lower temperatures, have curved and less well-defined facets. Inclusions with hep structure, the stable phase at room temperature, have not been observed.

Type
Research Article
Copyright
Copyright © Materials Research Society 1994

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References

REFERENCES

1 Johnson, E., Hjemsted, K., Schmidt, B., Bourdelle, K.K., Johansen, A., Andersen, H.H. and Sarholt-Kristensen, L., in Phase Formation and Modification by Beam-Solid Interactions MRS Symp. Proc, Vol. 235, edited by Was, G.S., Rehn, L.E. and Follstaedt, D.M. (Pittsburg PA, Materials Research Society, 1992), p. 485.Google Scholar
2 Johnson, E., Johansen, A., Thoft, N.B., Andersen, H.H. and Sarholt-Kristensen, L., Phil. Mag. Lett. 68 (1993) 131.Google Scholar
3 Massalski, T.B., Murray, J.L., Bennett, L.H. and Baker, H. (eds.), Binary Alloy Phase Diagrams, (Metals Park OH, American Society for Metals, 1986) p. 176.Google Scholar
4 Tonkov, E. Yu., High Pressure Phase Transformations. A Handbook, (Philadelphia PA, Gordon & Breach, 1992) Vol. 2, p. 683.Google Scholar
5 Christian, J.W., Metall. Trans. A, 21A (1990) 799.Google Scholar
6 Grey, F. and Bohr, J., Appl. Surf. Sci. 65/66 (1993) 35.Google Scholar
7 Hirsch, P.B., Howie, A., Nicholson, R.B., Pashley, D.W. and Whelan, M.J., Electron Microscopy of Thin Crystals (London, Butterworths 1965).Google Scholar
8 Saka, H., Nishikawa, Y. and Imura, T., Phil. Mag. A, 57 (1988) 895.Google Scholar
9 Gråbæk, L., Bohr, J., Andersen, H.H., Johansen, A., Johnson, E., Sarholt-Kristensen, L. and Robinson, I.K., Phys. Rev. B, 45 (1992) 2628.Google Scholar