2017
DOI: 10.1016/j.actamat.2017.04.039
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Pseudoelasticity and shape memory effects in cylindrical FCC metal nanowires

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Cited by 24 publications
(11 citation statements)
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“…Thus, the re-orientation of the Ag NW from (110) into a more preferred (100) (see Figure 4 ) phase, as also shown in Figure 3 a, conferred additional plasticity to the Ag NW. This behavior is reported in numerous studies [ 7 , 8 , 9 , 10 ] related to deformation in metallic nanowires. At elevated temperatures, the propagation of twin boundaries is retarded due to thermal vibrations and complete transformation from (110) to (100) phase is not possible.…”
Section: Results and Discussionsupporting
confidence: 72%
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“…Thus, the re-orientation of the Ag NW from (110) into a more preferred (100) (see Figure 4 ) phase, as also shown in Figure 3 a, conferred additional plasticity to the Ag NW. This behavior is reported in numerous studies [ 7 , 8 , 9 , 10 ] related to deformation in metallic nanowires. At elevated temperatures, the propagation of twin boundaries is retarded due to thermal vibrations and complete transformation from (110) to (100) phase is not possible.…”
Section: Results and Discussionsupporting
confidence: 72%
“…At the nanoscale, 1D NWs usually exhibit ultra high strength, differently from bulk materials, which makes them ideal candidates for studying their fundamental deformation mechanisms. Dislocation nucleation from free surfaces and its subsequent propagation through NWs has been found to be a dominant deformation mechanism in metallic NWs such as Au, Ag, Cu, and Ni [ 5 , 6 , 7 , 8 , 9 , 10 , 11 , 12 , 13 ]. This enables reorientation to a more preferred phase, resulting in exceptional mechanical properties such as superplasticity, high yielding strength, pseudoelasticity, and shape memory effects [ 5 , 6 , 7 , 8 , 9 ].…”
Section: Introductionmentioning
confidence: 99%
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“…In NWs, however, twin formation is not necessarily followed by dislocations slip, but rather by twinning on conjugate slip planes [27]. In our calculations, we observed a transition from twinning to full slip, in agreement with previous atomistic simulations [23,28]. This difference between experiments and simulations might be partly explained by the crystal re-orientation caused by twinning and the use of periodic boundary conditions in simulations, whereas experimentally NW ends are clamped.…”
Section: Au-nw At 300ksupporting
confidence: 83%