1977
DOI: 10.1080/14786437708232942
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The stacking-fault energy of nickel

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Cited by 255 publications
(64 citation statements)
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“…[21,22] In particular, the dissociation width of the edge dislocation is quantitatively well reproduced by this potential. In our simulations, the dissociation width equals 3.3 nm, which agrees with the observations of Carter and Holmes [23] who estimate this width, between 1.8 and 3.6 nm. For pure aluminum we chose the potential proposed by Voter and Chen, [24] which has the drawback of yielding a low stacking fault energy (compared e.g.…”
Section: Simulation Methods and Simulation Cellsupporting
confidence: 81%
“…[21,22] In particular, the dissociation width of the edge dislocation is quantitatively well reproduced by this potential. In our simulations, the dissociation width equals 3.3 nm, which agrees with the observations of Carter and Holmes [23] who estimate this width, between 1.8 and 3.6 nm. For pure aluminum we chose the potential proposed by Voter and Chen, [24] which has the drawback of yielding a low stacking fault energy (compared e.g.…”
Section: Simulation Methods and Simulation Cellsupporting
confidence: 81%
“…[30] The second stage corresponds to a roughly constant hardening rate h II . Multiple slips of dislocations then occur leading to the formation of cells of dislocations for materials with high stacking fault energy such as nickel (around 150 mJ/m 2 [31] ). It can be observed that h II strongly decreases with the thickness.…”
Section: A Work Hardening Evolution and Surface Effects Characterizamentioning
confidence: 99%
“…Transmission electron microscopy (TEM) imaging is widely used in that purpose, for it provides insight into individual defect configuration at the near atomic level. For instance, in the case of dislocations, TEM is used to size nanometric dissociation distances so as to obtain the stacking fault energy (Baluc and Schä ublin, 1996;Carter and Holmes, 1977;Hemker and Mills, 1993;Stobbs and Sworn, 1971) or to deduce the dislocation core configuration in ordered alloys (Kumar et al, 1999;Lang et al, 2004). In the case of radiation damage, the point defects, interstitials, vacancies or impurities, generated by the impinging energetic particles condense to form nanometric three-dimensional defects or clusters that eventually may transform in stacking fault tetrahedra (SFT), dislocation loops, cavities, which are voids when empty or bubbles when filled with a gas, or secondary phase precipitates.…”
Section: Introductionmentioning
confidence: 99%