1989
DOI: 10.4028/www.scientific.net/ssp.6-7.235
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Interaction of Point Defects with Interstitial Clusters, Dislocations and Impurities During in SITU Electron Irradiation of Silicon Crystals in the Electron Microscope

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Cited by 14 publications
(27 citation statements)
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“…The latter are known to be the result of the growth of rodlike defects under electron irradiation. 45,46 They are two-dimensional interstitial platelets and can be seen as interstitial-type dislocation loops lying on ͕311͖ planes in contrast to perfect loops or Frank loops that lie on ͕111͖ planes. They have been observed in the case of helium implantation in silicon at high temperature.…”
Section: Implantations At T I = 250°c and Annealingmentioning
confidence: 99%
“…The latter are known to be the result of the growth of rodlike defects under electron irradiation. 45,46 They are two-dimensional interstitial platelets and can be seen as interstitial-type dislocation loops lying on ͕311͖ planes in contrast to perfect loops or Frank loops that lie on ͕111͖ planes. They have been observed in the case of helium implantation in silicon at high temperature.…”
Section: Implantations At T I = 250°c and Annealingmentioning
confidence: 99%
“…A fundamental reason of this phenomenon is the existence of energy and/or entropy barriers for transition of self-interstitial atoms from a metastable site (IDCs) to a stable lattice site. For instance in the plane of dislocation loop the barrier is about 1.3 eV [1,2]. We assume that the height of this barrier for combined clustering of point defects depends on the initial atomic structure of the vacancy agglomerate.…”
Section: Introductionmentioning
confidence: 99%
“…This process has been studied in detail by in situ electron irradiation in a high voltage electron microscope (HVEM) at a wide temperature range between 20 and 1150 o C. Based upon clustering of very mobile Si i during electron irradiation, some of the coefficients of point defect reactions in Si (with dislocations, dopant atoms, and interfaces) have been determined [1]. An important conclusion is that the interaction coefficient of the less mobile vacancies with the real surface (or with surfaces capped with thin SiO 2 and Si 3 N 4 ) is much larger than that for interaction with Si i (up to two orders of magnitude).…”
Section: Introductionmentioning
confidence: 99%
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