2021
DOI: 10.1557/s43578-021-00261-y
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Effect of interface structure on dislocation glide behavior in nanolaminates

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Cited by 9 publications
(7 citation statements)
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“…The initial peak stress in both SC-Ag and FS-Ag is significantly lower than in the nanolaminated Ag, being around 4 MPa for SC-Ag and 5.7 MPa for FS-Ag. In a Cu single crystal, it was also found that the SC model has a lower critical stress than the FS model [ 14 ]. The primary resistance to dislocation motion in the SC-Ag comes from the lattice itself.…”
Section: Results and Discussionmentioning
confidence: 99%
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“…The initial peak stress in both SC-Ag and FS-Ag is significantly lower than in the nanolaminated Ag, being around 4 MPa for SC-Ag and 5.7 MPa for FS-Ag. In a Cu single crystal, it was also found that the SC model has a lower critical stress than the FS model [ 14 ]. The primary resistance to dislocation motion in the SC-Ag comes from the lattice itself.…”
Section: Results and Discussionmentioning
confidence: 99%
“…In these layers, the x , y , and z axes denote coordinates for layer M , while , , and pertain to layer . We have applied PBCs along the x (or ) and y (or ) axes, while traction-free boundary conditions are implemented along the z (or ) axis [ 14 , 47 , 48 , 49 ]. The crystallographic orientations are shown in Table 1 .…”
Section: Materials and Methodsmentioning
confidence: 99%
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“…To investigate the effect of interface structure on CLS motion, MD was applied to h = 5 nm Cu/Nb nanolaminates and nanotwinned Cu or Nb. Glide behavior was jerky for the semicoherent Cu/Nb interface, due to interactions with discrete misfit dislocation arrays in the interface (Figure 7b) (42). In contrast, the coherent interfaces in the nanotwinned material posed substantially less glide resistance, and CLS glide was smooth.…”
Section: Blocking and Restricting Dislocation Motionmentioning
confidence: 99%