“…Equations [1] and [2] show that for a perfect dislocation loop, the activation-energy barrier for nucleation will depend on the level of stress and the Burger's vector, whereas, for a partial dislocation loop, the activation-energy barrier for nucleation will depend on the SFE, in addition to and b P . Assuming the Burgers vector of a perfect dislocation, b 0 ϭ a/2 Ͻ110Ͼ ϭ 2.53 ϫ 10 Ϫ10 m, [13] where a is the lattice parameter of the austenite phase, the Burgers vector of a partial dislocation is b P ϭ a/6 Ͻ112Ͼ ϭ 1.46 ϫ 10 Ϫ10 m, [13] and the SFE is ␥ ϭ 0.020 J/m 2 , [14] we can plot the activation energy of nucleation (⌬G) for a perfect and for a partial dislocation loop, as a function of the loop radius.…”