The computer simulation of EBIC contrast of uncharged dislocation as a function of excitation level is carried out. It is shown, that if a real distribution of excess carriers is taken into account under calculations a smooth decay of dislocation contrast close to logarithmic one can be obtained even for uncharged dislocations.
IntroductionThe electron beam induced current (EBIC) measurements in the scanning electron microscope are now widely used to study the electrophysical properties of materials and microelectronic devices. The basic physical characteristic investigated by this method is the minority carrier diffusion length [1]. First applications of the EBIC method were associated with an evaluation of point defect concentration and with a characterization of 1D defects (dislocations) [2]. Recently the interest to the study of dislocation properties has increased due to attempts to realize the effective light-emitting devices on a basis of artificially created dislocation structures in silicon [3]. In the EBIC mode dislocations can be revealed as dark objects, that evidences the enhanced recombination rate in the region, adjacent to them. The dislocation recombination activity could be characterized by a value of maximum contrast in EBIC mode [2].It was shown experimentally [4] that in Si the dependence of dislocation EBIC contrast on beam current had a plateau at a small excitation level and with an increase of excitation level (beginning from some critical value I log ) a smooth decay close to the logarithmic one was observed over a several order change of beam current. The threshold value I log depends on the dopant concentration and sample temperature. The application of Shockley-Read-Hall electron-hole recombination model [5] without taking into account the real distribution of excess carriers leads to the conclusion, that the contrast decrease with increasing e-beam current should be rather sharp and the transition between the regions of low and high injection level occurs over one order of beam current variation only. As shown in [6] using the simple calculations, the logarithmic decay of the EBIC contrast with beam current increasing could be observed for charged dislocations. This model seems to be confirmed for n-Si, in which the logarithmic decrease of dislocation EBIC contrast [4] and evidences for 60º dislocation charging [7] were obtained. Therefore the logarithmic dependence of the EBIC contrast on beam current was considered in many works as an argument supporting the charge of dislocations under study.However, under the EBIC investigations in semiconductors with the large diffusion lengths (such as Si) a high excitation level is usually reached that could lead to an essential reduction of dislocation charge even if they are charged without an excitation. It was shown [8] that in Si the temperature dependence of dislocation EBIC contrast in many cases did not follow the predictions of charge dislocation