2004
DOI: 10.1002/pssa.200306819
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Defects in silicon plastically deformed at room temperature

Abstract: Positron trapping in silicon deformed under high‐stress conditions at room temperature is compared to that in Si plastically deformed at higher temperatures. After room temperature deformation, thermally rather stable vacancy clusters appear. No evidence for positron capture in dislocations is found. In contrast, after high‐temperature deformation, positrons are trapped in rather large vacancy clusters and in dislocations acting as combined positron traps. The specific features of positron trapping in silicon … Show more

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Cited by 8 publications
(3 citation statements)
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“…19. These clusters are not stable in view of results on Fz-Si plastically deformed at room temperature: 31 Vacancy clusters were formed that gave rise to a positron lifetime of 460 ps which was unaffected by annealing to ϳ800°C for 1 2 h, and the lifetime suggests an average size of 18 vacancies, nearly twice that found in this work.…”
Section: Samplementioning
confidence: 54%
“…19. These clusters are not stable in view of results on Fz-Si plastically deformed at room temperature: 31 Vacancy clusters were formed that gave rise to a positron lifetime of 460 ps which was unaffected by annealing to ϳ800°C for 1 2 h, and the lifetime suggests an average size of 18 vacancies, nearly twice that found in this work.…”
Section: Samplementioning
confidence: 54%
“…A pronounced maximum positron lifetime throughout the measuring temperature occurs after annealing at 600 • C. This maximum positron lifetime has been interpreted by dislocation motion and relaxing. The interaction of dislocations gives rise to the formation of new vacancies, which agglomerate to stable vacancy clusters [12]. At above 600 • C the stability limit of vacancy clusters is reached, and they start to decay by a big margin so a distinct annealing stage occurs at above 700 • C.…”
Section: Experimental Details and Resultsmentioning
confidence: 99%
“…We need to systemize these equations before fitting the associated parameters because of the regular format of the language in Matlab. The positron lifetime in the defect-free bulk τ b is 218 ps, and for the other two positron lifetimes τ t is 300 ps [11] and τ st is 240 ps; besides we fix τ viod to 500 ps [12] . So four kinds of positron annihilation rates can be calculated as…”
Section: Experimental Data Processingmentioning
confidence: 99%