Hostname: page-component-cd9895bd7-8ctnn Total loading time: 0 Render date: 2024-12-27T02:10:39.314Z Has data issue: false hasContentIssue false

Preliminary First Principles Study Of Hf and Zr Aluminates as Replacement High-k Dielectrics

Published online by Cambridge University Press:  21 March 2011

Michael Haverty
Affiliation:
Materials Science and Engineering, Stanford University, Stanford, CA 94305, U.S.A. Multiscale Simulation Laboratory, Stanford University, Stanford, CA 94305, U.S.A.
Atsushi Kawamoto
Affiliation:
Center For Integrated Systems, Stanford University, Stanford, CA 94305, U.S.A.
Gyuchang Jun
Affiliation:
Materials Science and Engineering, Stanford University, Stanford, CA 94305, U.S.A. Multiscale Simulation Laboratory, Stanford University, Stanford, CA 94305, U.S.A.
Kyeongjae Cho
Affiliation:
Multiscale Simulation Laboratory, Stanford University, Stanford, CA 94305, U.S.A.
Robert Dutton
Affiliation:
Center For Integrated Systems, Stanford University, Stanford, CA 94305, U.S.A.
Get access

Abstract

Bulk Density Functional Theory calculations were performed on Hf and Zr substitutions for Al in κ-alumina. The lowest energy configuration found was an octahedrally coordinated Zr site. Zr dissolution was favorable with an enthalpy of -2eV/unit cell for forming Al1.875Zr0.125O3 from pure Zr and κ-alumina. Hf and Zr substitution for Al atoms introduced empty d-states below the conduction band edge reducing the Eg of pure κ-alumina (7.5eV) to 6.4-5.9eV. The edge of the valence band however remained fixed by the O p-state character. The substitution of Hf and Zr into the alumina structure may lead to a higher dielectric constant, but will also reduce Eg and result in a trade off in tunneling currents in devices.

Type
Research Article
Copyright
Copyright © Materials Research Society 2001

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

REFERENCES

1 Wilk, G. D. and Wallace, R. M., Appl. Phys. Lett. 76 (1) 112, (2000).Google Scholar
2 Wilk, G. D., Wallace, R. M., and Anthony, J. M., Journal of App. Phys. 87 (1) 484, (2000).Google Scholar
3 Guzev, E. P., Copel, M., and Cartier, E., Appl. Phys. Lett. 76 (2) 176, 2000.Google Scholar
4 Kawamoto, A., Jameson, J., Cho, K., and Dutton, R., IEEE Trans. On Elec. Dev. 47 (10) 1787, (2001).Google Scholar
5 Jun, G., Cho, K., and Dutton, R., Semiconductor Research Corp. Deliverables Report, (2001).Google Scholar
6 Hohenberg, P. and Kohn, W., Phys. Rev. B., 136 [3] B864–B871, (1964).Google Scholar
7 Kohn, W. and Sham, L. J., Phys. Rev. A., 140 [4] A1133–A1138, (1965).Google Scholar
8VASP (Vienna Ab-initio Simulation Package) is commercial licensed through the Theoretical Physics Department at the University of Vienna, Austria.Google Scholar
9 Daviero, S., Ibanez, A., Avinens, C., Flank, A.M., Thin Solid Films, 226[2] 207, (1993)Google Scholar
10 Dupree, R., Farnan, I., Forty, A.J., El-Mashri, S., J. de Phys. Coll., 46 [C-8] p.113–17, (1985).Google Scholar
11 Yourdshahyan, Y., Ruberto, C., Halvarsson, M., Bengtsson, L., Langer, V., and Lundqvist, B., J. Am. Ceram. Soc. 82 [6] 1365–80, (1999).Google Scholar
12 Ollivier, B., Retoux, R., Lacorre, P., Massiot, D., J. Mater. Chem. 7 [6] 10491056, (1997).Google Scholar
13 Kittel, C., Intro. to Solid State Physics, 7th ed. (John Wiley and Sons, New York, 1996) p. 57.Google Scholar
14Http://www.webelements.com/webelements/elements/text/Al/radii.html and Http://www.webelements.com/webelements/elements/text/Zr/radii.html.Google Scholar
15 Kawamoto, A., Jameson, J., Griffin, P., Cho, K., and Dutton, R., IEEE Elec. Device Lett. 22 [1] 1416, (2001).Google Scholar