2005
DOI: 10.1016/j.nimb.2004.12.038
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Channeling characterization of defects in silicon: an atomistic approach

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Cited by 15 publications
(6 citation statements)
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“…For silicon, it was shown using computer simulations that certain point defects lead to the displacement of up to 9 atoms (9 displaced atoms were found for <110>-split interstitials and 4 for vacancies). 26 In the case of GaAs, the number of displaced atoms per Frenkel pair was estimated experimentally to be 14±4 in weakly damaged material. 27 (viii) The presence of dislocations may be considered within the framework of the Peierls-Nabarro model of edge dislocations (DIS).…”
Section: (V)mentioning
confidence: 99%
“…For silicon, it was shown using computer simulations that certain point defects lead to the displacement of up to 9 atoms (9 displaced atoms were found for <110>-split interstitials and 4 for vacancies). 26 In the case of GaAs, the number of displaced atoms per Frenkel pair was estimated experimentally to be 14±4 in weakly damaged material. 27 (viii) The presence of dislocations may be considered within the framework of the Peierls-Nabarro model of edge dislocations (DIS).…”
Section: (V)mentioning
confidence: 99%
“…͑2͒ with RBS/C data, one has to connect the defect concentration c r to the relative displaced fraction s through a RBS/C defect scattering function, s͑c r ͒, that may depend on the specific defect structure. Recent calculations 21 have provided the shape of this function for several defect structures in silicon. In the case of LiNbO 3 , such information is not available and, therefore, one is forced to make some convenient approximations on the function s͑c r ͒ to perform a meaningful analysis of the data and particularly learn about the transition from the isolated defect ͑preamorphous͒ region to the amorphous region.…”
Section: General Phenomenological Descriptionmentioning
confidence: 99%
“…Therefore, one has to derive such information through a suitable scattering function that relates the RBS/C response to the defect concentration. 21 Then, one obtains the evolution of defect concentration with the irradiation fluence. The results are finally analyzed within a very general context, and the validity of the various theoretical approaches is comparatively assessed.…”
Section: Introductionmentioning
confidence: 99%
“…To analyze the cause of this difference, we have plotted the radius at which the defect concentration falls below 1% as measured from the center of the track in figure 4. This threshold was chosen based on a reasonable error limit in a RBS-c experiment [54] in defect sensitivity for a qualitative comparison. It can be seen that at high stopping powers, the defected track extends to a notably larger region than the one with density fluctuations.…”
mentioning
confidence: 99%