Hiroshi Ito, Reinhold Schwalm
JES
a〈1 0 0〉 Dislocations are observed in nickel-base superalloys after creep deformation at high temperatures and low stresses. They are formed in the γ/γ′ interfaces by a three step mechanism. First, primary dislocations with Burgers vector a/2〈1 0 1〉 and 60° character are left behind in the interfaces when dislocation loops glide through the γ channels. The 60° dislocations move into edge orientation and react forming secondary dislocations a/2〈1 1 0〉. In the third step, new primary dislocations are knit into the already existing meshes of primary and secondary dislocations, which results in hexagonal misfit dislocation networks consisting of secondary dislocations a/2〈1 1 0〉 and tertiary dislocations a〈1 0 0〉, both of edge type. This self-organisation process is explained by dislocation theory and crystallography. Creep deformation accelerates when the a〈1 0 0〉 interfacial dislocations enter the γ′ phase. During their climb towards the opposite interface, they attain a characteristic rectangular shape. This shape and the importance of the a〈1 0 0〉 super dislocations for creep deformation are discussed. © 2005 Elsevier B.V. All rights reserved.
Hiroshi Ito, Reinhold Schwalm
JES
Kenneth R. Carter, Robert D. Miller, et al.
Macromolecules
A. Gangulee, F.M. D'Heurle
Thin Solid Films
T.N. Morgan
Semiconductor Science and Technology