2013
DOI: 10.1063/1.4793635
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Shuffle-glide dislocation transformation in Si

Abstract: The transformation of dislocation cores from the shuffle to the glide set of {111} glide planes in Si is examined in this work. The transformation is thermally activated and is favored by a resolved shear stress which applies no force on the original perfect shuffle dislocation. A resolved shear stress driving dislocation motion in the glide plane is not observed to promote the transition. The stress-dependent activation energy for the described shuffle-glide transformation mechanism is evaluated using a stati… Show more

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Cited by 21 publications
(14 citation statements)
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“…Earlier reports analytically estimate K C for nano and microlength scale samples within a limited temperature range of 60–80 °C. ,, Our results show that the crack tip shielding mechanism in the form of crack branching begins to operate in SC Si at intermediate temperatures between 300 and 400 °C (Figure f,h and c), which is considerably lower compared to the reported BDTT of macro-Si. This could be due to activation of partial dislocation slip at these temperatures . Silicon has a diamond cubic structure, which is equivalent to two interpenetrating FCC lattices shifted by a /4⟨111⟩.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Earlier reports analytically estimate K C for nano and microlength scale samples within a limited temperature range of 60–80 °C. ,, Our results show that the crack tip shielding mechanism in the form of crack branching begins to operate in SC Si at intermediate temperatures between 300 and 400 °C (Figure f,h and c), which is considerably lower compared to the reported BDTT of macro-Si. This could be due to activation of partial dislocation slip at these temperatures . Silicon has a diamond cubic structure, which is equivalent to two interpenetrating FCC lattices shifted by a /4⟨111⟩.…”
Section: Resultsmentioning
confidence: 99%
“…Silicon has a diamond cubic structure, which is equivalent to two interpenetrating FCC lattices shifted by a /4⟨111⟩. This results in loss of symmetry along the {111} planes, the planes of easy slip in FCC materials, resulting in slip being accommodated by two asymmetric glide and shuffle planes . The glide plane can accommodate slip via disassociated partials in addition to activating full dislocations at high temperatures, while the shuffle plane can only accommodate full dislocations.…”
Section: Resultsmentioning
confidence: 99%
“…At last, the formation of the peculiar partial dislocations for <111> compression is probably correlated to large and inhomogeneous stresses, although the exact relationship is difficult to extract. It is interesting that recently, Li and Picu showed that a suitable stress state could promote the dissociation of perfect shuffle into glide partial dislocations [69].…”
Section: Discussionmentioning
confidence: 99%
“…[ 24 ] The compact dislocation cores in Type I interface and the extended dislocation cores in the other two types of interface are consistent with the fact that, at low temperatures, dislocations in Si have compact and extended cores, respectively, when they are in the shuffle‐set and glide‐set slip planes. [ 48 ] Recent experiments and atomistic simulations found that within the Al/Si (111) interface that coincides with the glide‐set slip plane in Si, there are two domains with threefold and sixfold symmetries, respectively. [ 49 ] These two domains, respectively, similar to Type II and Type III interfaces identified in our work, allow for complete relaxation of the misfit strain.…”
Section: Resultsmentioning
confidence: 99%