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

1997 ◽  
Vol 469 ◽  
Author(s):  
S. Libertino ◽  
J. L. Benton ◽  
S. Coffa ◽  
D. C. Jacobson ◽  
D. J. Eaglesham ◽  
...  

AbstractWe 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 annealing 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 1×109 to 1010/cm2) and electron irradiated (9.2 MeV to fluences between 1 and 3×1015/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 ◽  
Vol 469 ◽  
Author(s):  
J. L. Benton ◽  
S. Libertino ◽  
S. Coffa ◽  
D. J. Eaglesham

ABSTRACTWe have investigated the properties of Si interstitial clusters in ion implanted crystalline Si. Deep Level Transient Spectroscopy measurements have been used to characterize the residual damage in Si samples implanted with Si ions at fluence in the range 1×109-1×1012/cm2 and annealed at temperatures of 100–700 °C. We have found that, in the fluence and annealing temperature range where extended defects are not formed, the residual damage is dominated by Si interstitial clusters which introduce deep levels at Ev+0.36 eV and at Ev+O-53 eV. By using Si substrates with a different impurity and dopant content, we have found that C, O and B play a role in determining the defect growth kinetics but are not the main constituents of these clusters. We estimate that 40 to 125 Si self intersti-tials are stored in these clusters and believe that they are the main source of Si self-inter-stitials in transient enhanced diffusion phenomena occurring in the absence of {311} or extended defects.


1991 ◽  
Vol 223 ◽  
Author(s):  
A. Vaseashta ◽  
L. C. Burton

ABSTRACTKinetics of persistent photoconductivity, photoquenching, and thermal and optical recovery observed in low energy Ar+ bombarded on (100) GaAs surfaces have been investigated. Rate and transport equations for these processes were derived and simulated employing transport parameters, trap locations and densities determined by deep level transient spectroscopy. Excellent correlation was obtained between the results of preliminary simulation and the experimentally observed values. The exponential decay of persistent photoconductivity response curve was determined to be due to metastable electron traps with longer lifetime and is consistent with an earlier proposed model.


2003 ◽  
Vol 762 ◽  
Author(s):  
M. Zeman ◽  
V. Nádaždy ◽  
R.A.C.M.M. van Swaaij ◽  
R. Durný ◽  
J.W. Metselaar

AbstractThe charge deep-level transient spectroscopy (Q-DLTS) experiments on undoped hydrogenated amorphous silicon (a-Si:H) demonstrate that during light soaking the states in the upper part of the gap disappear, while additional states around and below midgap are created. Since no direct correlation is observed in light-induced changes of the three groups of states that we identify from the Q-DLTS signal, we believe that we deal with three different types of defects. Positively charged states above midgap are related to a complex formed by a hydrogen molecule and a dangling bond. Negatively charged states below midgap are attributed to floating bonds. Various trends in the evolution of dark conductivity due to light soaking indicate that the kinetics of light-induced changes of the three gap-state components depend on their initial energy distributions and on the spectrum and intensity of light during exposure.


1996 ◽  
Vol 438 ◽  
Author(s):  
S. Libertino ◽  
S. Coffa ◽  
V. Privitera ◽  
F. Priolo

AbstractWe used deep level transient spectroscopy to determine the concentration and depth profile of the defects introduced by MeV He and Si implants in n-type crystalline Si. We have found that only ∼ 16% of the Frenkel pairs generated by the ion escapes recombination and is stored into room temperature stable defects such as divacancies and oxygen vacancy complexes. For a light ion (He), the depth distribution of these defect complexes is strongly dependent on the O content of the substrate: it mirrors the initial distribution of I-V pairs, as calculated by TRIM (a Monte Carlo Code) when the O content is high (∼ 1018/cm3) while it can be much wider (up to 2 μm) in a highly pure (low O content) epitaxial substrate. This effect is due to a long range migration of vacancies before clustering or trapping at impurities. This migration is strongly inhibited for an ion of higher mass (such as Si) since in a denser collision cascade direct clustering is strongly favoured with respect to agglomeration of migrating defects.


1989 ◽  
Vol 158 ◽  
Author(s):  
Zheng Xu ◽  
Toshihiko Kosugi ◽  
Kenji Gamo ◽  
Susumu Namba

ABSTRACTW films were deposited on n-GaAs by ion beam assisted deposition technique using low energy H2+ and Ar+, and film properties and residual damage in the substrate were investigated by measuring X-ray photoemission, current-voltage characteristics and deep level transient spectroscopy. Films with a resistivity of 1O−5 ohm·cm were formed. It was observed that damage can be reduced using the low energy beams and that Schottky contacts with n-factor of almost 1 and barrier height of 0.88 eV were formed.


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