Skip to main content
Log in

Nickel silicide as a contact material for submicron CMOS devices

  • Special Issue Paper
  • Published:
Journal of Electronic Materials Aims and scope Submit manuscript

Abstract

Nickel monosilicide (NiSi) is an attractive alternative to the currently used silicides for the coming generations of deep submicron complementary metaloxide-semiconductor (CMOS) devices. This silicide material has a resistivity, which is comparable to that of TiSi2 or CoSi2, but consumes less silicon for its formation. The silicide silicon interface is relatively planar and, unlike TiSi2, its resistivity does not change with the linewidth for narrow lines. However, the thermal stability of NiSi is relatively poor at the currently used temperatures during process integration. Recent studies have shown that the stability of these films could be increased substantially through the small addition of alloy elements, which do not increase the resistivity of the NiSi film. Morever, it has been demonstrated that the addition of a small amount of alloy elements significantly reduces diode leakage, possibly due to the suppression of silicide spike formation as a result of alloy addition. This paper will present and discuss the details of these experimental results.

This is a preview of subscription content, log in via an institution to check access.

Access this article

Price excludes VAT (USA)
Tax calculation will be finalised during checkout.

Instant access to the full article PDF.

Similar content being viewed by others

References

  1. T. Ohguro, S. Nakajima, M. Koike, T. Morimoto, A. Nishiyama, Y. Ushiku, T. Yoshitomi, M. Ono, M. Saito, and H. Iwai, IEEE Trans. Electron Devices 42, 2305 (1994).

    Article  Google Scholar 

  2. F. Deng, R.A. Johnson, P.M. Asbeck, S.S. Lau, W.B. Dubbelday, T. Hsiao, and J. Woo, J. Appl. Phys. 81, 8047 (1997).

    Article  CAS  Google Scholar 

  3. R. Mukai, S. Ozawa, and H. Yagi, Thin Solid Films 270, 567 (1995).

    Article  CAS  Google Scholar 

  4. D. Mangelinck, J.Y. Dai, S.K. Labiri, C.S. Ho, K.L. Pey, and T. Osipowicz, MRS Spring Meeting Warrendale, PA: MRS, 1999).

    Google Scholar 

  5. Klaus, Graff, Metal Impurities in Silicon-Device Fabrication, Springer Series in Materials Science, Springer, NY, p. 75–82 (1995).

    Google Scholar 

  6. P.J. Grunthaner, F.J. Grunthaner, and A.J. Madhukar, J. Vac. Sci. Technol. 20, 680 (1982).

    Article  CAS  Google Scholar 

  7. F.M. d'Heurle, C.S. Petersson, J.E.E. Baglin, S. LaPlaca, and C.Y. Wong, J. Appl. Phys. 55, 4208 (1984).

    Article  Google Scholar 

  8. J. Barto;abs and L. Tesar; Phys. Status Solidi A 122, 607 (1990)

    Article  Google Scholar 

  9. S. Tanaka, K. Matsushita, and H. Kitagawa, Jpn. J. Appl. Phys. Part 1 35, 4624 (1996).

    Article  CAS  Google Scholar 

  10. Y.K. Kwon, T. Ishikawa, and H. Kuwano, J. Appl. Phys. 61, 1055 (1987).

    Article  CAS  Google Scholar 

  11. K.S.R.K. Rao, S.V. Pandu, Rangaiah, P.N. Reddy, and B.P.N. Reddy, J. Appl. Phys. 85, 2175, (1999).

    Article  CAS  Google Scholar 

  12. M. Seibt and W. Schröter, Phil. Mag. A. 59, 337 (1989).

    CAS  Google Scholar 

  13. B. Laurent, D. Mangelinck, B. Pichaud, A. Lhote, and J.B. Quorin, Solid State Phenom. 37–38, 157 (1994).

    Article  Google Scholar 

  14. M. Liehr, P.E. Schmid, F.K. LeCones, and P.S. Ho, Phys. Rev. Lett. 54, 2139 (1985).

    Article  CAS  Google Scholar 

  15. Because the forward current in good diodes is dominated by electron diffusion in the p+ neutral region, the saturation current Is can be expressed by Is=AqDnnpo/WP+, where A is the diode junction area, q is the electron charge, Dn is electron diffusion coefficient, npo is equilibrium electron concentration in the p+ regions, and Wp+ is the width of the p+ neutral region. Noting Dn α Tμ n and npo α T3 exp (−Eg/KT) and also that, for high dopant concentration Na (1018−1019 cm−3), the electron mobility μn is almost independent of temperature in the neightborhood of 300 K, the temperature dependence of saturation current is given by Is α T4 exp (−Eg/KT) with Eg as the bandgap and K as the Boltzmann constant.

  16. F.A. Padovani and R. Stratton Solid-State Electron. 9, 695 (1966).

    Article  Google Scholar 

Download references

Author information

Authors and Affiliations

Authors

Rights and permissions

Reprints and permissions

About this article

Cite this article

Chi, D.Z., Mangelinck, D., Zuruzi, A.S. et al. Nickel silicide as a contact material for submicron CMOS devices. J. Electron. Mater. 30, 1483–1488 (2001). https://doi.org/10.1007/s11664-001-0162-4

Download citation

  • Received:

  • Accepted:

  • Issue Date:

  • DOI: https://doi.org/10.1007/s11664-001-0162-4

Key words

Navigation