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Oxygen vacancy defects in tantalum pentoxide: a density functional study

Published online by Cambridge University Press:  11 February 2011

R. Ramprasad
Affiliation:
Motorola Semiconductor Products Sector, 2100 E. Elliot Rd., Tempe, AZ 85284
Michael Sadd
Affiliation:
Motorola Semiconductor Products Sector, 3501 Ed Bluestein Blvd, Austin, TX 78721
Doug Roberts
Affiliation:
Motorola Semiconductor Products Sector, 3501 Ed Bluestein Blvd, Austin, TX 78721
Tom Remmel
Affiliation:
Motorola Semiconductor Products Sector, 2100 E. Elliot Rd., Tempe, AZ 85284
Mark Raymond
Affiliation:
Motorola Semiconductor Products Sector, 2100 E. Elliot Rd., Tempe, AZ 85284
Eric Luckowski
Affiliation:
Motorola Semiconductor Products Sector, 3501 Ed Bluestein Blvd, Austin, TX 78721
Sriram Kalpat
Affiliation:
Motorola Semiconductor Products Sector, 3501 Ed Bluestein Blvd, Austin, TX 78721
Carole Barron
Affiliation:
Motorola Semiconductor Products Sector, 3501 Ed Bluestein Blvd, Austin, TX 78721
Mel Miller
Affiliation:
Motorola Semiconductor Products Sector, 2100 E. Elliot Rd., Tempe, AZ 85284
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Abstract

First principles total energy calculations were performed in order to characterize O vacancy defects in Ta2O5. A simplified version of the crystalline orthorhombic phase of Ta2O5 was used in this study. Results indicate that O vacancies in Ta2O5 can be broadly classified based on their location in the lattice. One type of vacancies (occupying the “in-plane” sites) displays deep or mid gap occupied states, and shallow unoccupied states, while a second type (occupying “cap” sites) results in shallow occupied states. For a wide range of local Fermi level or chemical potential, the neutral and +2 charged states of the in-plane type vacancy and the +2 charge state of the cap type vacancy are found to be most stable. Migration energies of the two types of vacancies in the neutral and +2 charge states are markedly different, with the “cap” type of vacancies displaying very high barriers to migration (∼ 5 eV) compared to the “in-plane” type (∼ 0.5–1.0 eV).

Type
Research Article
Copyright
Copyright © Materials Research Society 2003

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References

REFERENCES

[1] Chaneliere, C., Autran, J. L., Devine, R. A. B., and Balland, B., Mater. Sci. Eng. R22, 269 (1998).Google Scholar
[2] Stephenson, N. C. and Roth, R. S., Acta. Cryst. B27, 1037 (1971).Google Scholar
[3] Kresse, G. and Hafner, J., Phys. Rev. B 47, 558 (1993); Phys. Rev. B 54, 11169 (1996).Google Scholar
[4] Foster, A. S., Sulimov, V. B., Lopez Gejo, F., Shluger, A. L., and Nieminen, R. M., Phys. Rev. B64, 224108 (2001).Google Scholar
[5] Yokozawa, Ayumi and Miyamoto, Yoshiyuki, Phys. Rev. B 55, 13783 (1997).Google Scholar
[6] Kimura, Hidekazu, Mizuki, Junichiro, Kamiyama, Satoshi, and Suzuki, Hiroshi, Appl. Phys. Lett. 66, 2209 (1995).Google Scholar
[7] Foster, A. S., Lopez Gejo, F., Shluger, A. L., and Nieminen, R. M., Phys. Rev. B 65, 174117 (2002).Google Scholar
[8] Fleming, R. M. et al, J. Appl. Phys. 88, 850 (2000).Google Scholar