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Defect Tails in GE Implanted Si Probed by Slow Positrons and Ion Channeling

Published online by Cambridge University Press:  10 February 2011

A P Knights
Affiliation:
School of Electronic Engineering, Information Technology and Mathematics, University of Surrey, Guildford GU2 5XH, United Kingdom. a.knights@ee.surrey.ac.uk
A Nejim
Affiliation:
School of Electronic Engineering, Information Technology and Mathematics, University of Surrey, Guildford GU2 5XH, United Kingdom. a.knights@ee.surrey.ac.uk
N P Barradas
Affiliation:
School of Electronic Engineering, Information Technology and Mathematics, University of Surrey, Guildford GU2 5XH, United Kingdom. a.knights@ee.surrey.ac.uk
R Gwilliam
Affiliation:
School of Electronic Engineering, Information Technology and Mathematics, University of Surrey, Guildford GU2 5XH, United Kingdom. a.knights@ee.surrey.ac.uk
P G Coleman
Affiliation:
School of Physics, University of East Anglia, Norwich, NR4 7TJ, United Kingdom.
F Malik
Affiliation:
School of Physics, University of East Anglia, Norwich, NR4 7TJ, United Kingdom.
H Kherandish
Affiliation:
MATS UK, Innovation House, Daten Park, Warrington, WA3 6UT, United Kingdom.
S Romani
Affiliation:
MATS UK, Innovation House, Daten Park, Warrington, WA3 6UT, United Kingdom.
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Abstract

Positron annihilation spectroscopy has been used to profile the distribution of defects following implantation of 120keV Ge+ into (100) Si in the dose range l x 1010 - lx104 cm−2 . The openvolume defect profiles can be adequately fitted assuming a simple rectangular block distribution extending to 350nm. Using anodic oxidation and etching, a procedure is described which allows details of the defect tails beyond the range of the implanted ion, usually inaccessible to positron -2 annihilation measurements, to be determined. For a time averaged dose-rate (Jr) of 0.02μA cm−2 and incident angle of 7°, open-volume defects are found to exist at concentrations exceeding 1016cm−3 at depths upto 600nm whereas the peak of the depth distribution of the implanted ions (Rp) is 76nm, measured using SIMS. When the time-average dose-rate is increased by a factor of 10, defects persist at concentrations in excess of 1017cm−3 beyond lμm and the Rp increases to 101nm. The open-volume defect profiles are compared to those deduced from Rutherford backscattering-channeling using the fitting routine DICADA.

Type
Research Article
Copyright
Copyright © Materials Research Society 1998

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References

REFERENCES

[1] Chason, E, Picraux, S T, Poate, J M, Borland, J O, Current, M I, Rubia, T Diaz de la, Eaglesham, D J, Holland, O W, Law, M E, Magee, C W, Mayer, J W, Melngallis, J, and Tasch, A F, J.Appl. Phys., 81, 6513 (1997).Google Scholar
[2] Lombardo, S, Pinto, A, Raineri, V., Larosa, P Ward G, Privitera, G, and Campisano, S U, Elec. Dev. Lett., 17, 485 (1996).Google Scholar
[3] Fahey, P M, Griffin, P B, and Plummer, J D, Rev. Mod. Phys., 61, 289, (1989).Google Scholar
[4] Asoka-Kumar, P, Lynn, K G, and Welch, D O, J. Appl. Phys., 76, 4935, (1994).Google Scholar
[5] Fujinami, M and Chilton, N B, J.Appl. Phys., 73, 3242, (1993).Google Scholar
[6] Fujinami, M, Tsuge, A, and Tanaka, K, J.Appl. Phys., 79, 9017, (1996).Google Scholar
[7] Knights, A P, Carlow, G R, Zinke-Allmang, M and Simpson, P J, Phys. Rev. B, 54, 13 955 (1996).Google Scholar
[8] Gdrtner, K., Nucl. Instr. and Meth. B, 132, 147 (1997).Google Scholar
[9] Aers, G C, in Positron Beams for solids and surfaces, Schultz, P J, Massoumi, G R and Simpson, P J, AIP conf. proc. 218, New York, (1990) p 162.Google Scholar
[10] Omri, M, Bonafos, C, Claverie, A, Nejim, A, Cristiano, F, Alquier, D, Martinez, A, and Cowern, N E B, Nucl. Inst. Meth. B, 120, 5, (1996).Google Scholar
[11] Nejim, A, Knights, A P, Jeynes, C, Coleman, P G, Patel, C J J. Appl. Phys., 83, 3565 (1998).Google Scholar
[12] Ziegler, J F, Biersack, J P, and Littmark, U, The stopping and range of ions in solids, Pergamon, New York, (1985).Google Scholar
[13] Al-Hashmi, S A R and Carter, G R, Rad. Effects, 102, 83 (1986).Google Scholar
[14] Berti, M, Drigo, A V, Lulli, G, Merli, P G, and Antisari, M Vittori, Phys. Stat. Sol., 97, 77 (1986).Google Scholar
[15] Williams, J S, Tan, HH, Goldberg, R D, Brown, R A, and Jagadish, C, Mat. Res. Soc. Symp. Proc., 316, 15 (1994).Google Scholar