2005
DOI: 10.1016/j.actamat.2005.04.012
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Nucleation of dislocations from [001] bicrystal interfaces in aluminum

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Cited by 196 publications
(82 citation statements)
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“…This deformation mechanism was obvious in many simulation works [14][15][16][17][18][19] , and it was also confirmed by in situ transmission electron microscopy (TEM) experiments 20,21 which showed GBs emitting partial dislocations that formed stacking faults and deformation twins in nanocrystalline Al and Cu. However, experiments at a nanoscale can be very time consuming and costly, and TEM requires samples with a thickness comparable to the grain size, which may induce the structure to relax and thus change the GB structure 1 , so they are very difficult to perform.…”
Section: Introductionmentioning
confidence: 76%
“…This deformation mechanism was obvious in many simulation works [14][15][16][17][18][19] , and it was also confirmed by in situ transmission electron microscopy (TEM) experiments 20,21 which showed GBs emitting partial dislocations that formed stacking faults and deformation twins in nanocrystalline Al and Cu. However, experiments at a nanoscale can be very time consuming and costly, and TEM requires samples with a thickness comparable to the grain size, which may induce the structure to relax and thus change the GB structure 1 , so they are very difficult to perform.…”
Section: Introductionmentioning
confidence: 76%
“…Recent MD simulations have revealed that looplike dislocations nucleate from GBs ͑or the leading partial comes from the GB, but the trailing partial on the same plane arises from the stacking fault left behind by the leading partial͒, 21 or from TBs. 22 This scenario for the formation of dislocation loops is somewhat different from that in conventional coarsegrained metals. For the latter materials, dislocation loops often form from Frank-Read sources inside the grains.…”
mentioning
confidence: 95%
“…Since the crystallographically constructed computational cells may not be in equilibrium, pre-loading relaxations are carried out to obtain their free standing configurations. Following this initial equilibration, approximate quasi-static tensile loading in each deformation increment is achieved though successive loading (at a specified rate of 0.005/ps) and equilibration steps (for 3 ps) using a combination of algorithms for NPT (Melchionna et al, 1993;Spearot et al, 2005) and NVE ensembles (Haile, 1997). The loading process results in a longitudinal strain increment of 0.25% (dilatation increment of $0.75%) per deformation increment.…”
Section: Computational Frameworkmentioning
confidence: 99%