We have investigated the defect structure of ion-implanted and electron irradiated crystalline Si using deep level transient spectroscopy measurements to characterize both vacancy-(V) and interstitial- (I) type defects and to monitor their evolution upon anneal-ing at temperatures <= 600 °C. It is found that only 4% of the Frenkel pairs generated by the energetic particles escape direct recombination and are stored into an equal number of room temperature stable V- and I-type defect complexes. No difference is found in the defect structure and annealing kinetics of ion implanted (1.2 MeV Si to fluences between 1x109 to 1010/cm2) and electron irradiated (9.2 MeV to fluences between 1 and 3x1015/cm2) samples in spite of the fact that denser collision cascades are produced by the ions. Annealing treatments result in a concomitant reduction in the concentration of I and V-type defects, demonstrating that defect recombination occurs preferentially in the bulk and not at the sample surface. Finally, at temperature above 300 °C, when most of the vacancy-type defects have been recombined, a residual concentration of I-type defects is found in ion implanted samples. This interstitial excess, not detected in electron irradiated samples, provides a direct evidence of the imbalance between I and V concentration produced by the extra incorporated ion.

The effect of the extra ion on residual damage in MeV implanted Si

S Libertino;M Lavalle;
1997

Abstract

We have investigated the defect structure of ion-implanted and electron irradiated crystalline Si using deep level transient spectroscopy measurements to characterize both vacancy-(V) and interstitial- (I) type defects and to monitor their evolution upon anneal-ing at temperatures <= 600 °C. It is found that only 4% of the Frenkel pairs generated by the energetic particles escape direct recombination and are stored into an equal number of room temperature stable V- and I-type defect complexes. No difference is found in the defect structure and annealing kinetics of ion implanted (1.2 MeV Si to fluences between 1x109 to 1010/cm2) and electron irradiated (9.2 MeV to fluences between 1 and 3x1015/cm2) samples in spite of the fact that denser collision cascades are produced by the ions. Annealing treatments result in a concomitant reduction in the concentration of I and V-type defects, demonstrating that defect recombination occurs preferentially in the bulk and not at the sample surface. Finally, at temperature above 300 °C, when most of the vacancy-type defects have been recombined, a residual concentration of I-type defects is found in ion implanted samples. This interstitial excess, not detected in electron irradiated samples, provides a direct evidence of the imbalance between I and V concentration produced by the extra incorporated ion.
1997
Istituto per la Microelettronica e Microsistemi - IMM
Inglese
T. Diaz de la Rubia, S. Coffa, P. A. Stolk and C. S. Rafferty
DEFECTS AND DIFFUSION IN SILICON PROCESSING
Symposium on Defects and Diffusion in Silicon Processing
187
192
6
1-55899-373-8
Sì, ma tipo non specificato
APR 01-04, 1997
San Francisco (USA)
3
none
S. Libertino; J. L. Benton; S. Coffa; D.C. Jacobson; D. J. Eaglesham; J. M. Poate; M. Lavalle; P.G. Fuochi
273
info:eu-repo/semantics/conferenceObject
04 Contributo in convegno::04.01 Contributo in Atti di convegno
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/20.500.14243/134443
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