Skip to main content
. 2021 Aug 16;121(16):10073–10141. doi: 10.1021/acs.chemrev.1c00022

Figure 30.

Figure 30

Applications of GAP to α-iron, from small unit cells (left) to large-scale simulations (right). (a) Energy for the Bain path, corresponding to the distortion of a body-centered cubic (bcc) unit cell to give tetragonal cells including one corresponding to a face-centered cubic (fcc) structure, as indicated. The results of spin-polarized DFT calculations for different magnetizations are shown, together with the prediction of a GAP model fitted to data corresponding to the ferromagnetic state. The GAP predicted error, indicated by shading, is mostly smaller than the line width, except around the Inline graphic ratio corresponding to an fcc structure. Reprinted figure with permission from ref (241). Copyright 2017 by the American Physical Society. (b) Simulation setup for the computation of the double-kink nucleation barrier of a screw dislocation in a large periodic supercell model; details are given in ref (242). Adapted from ref (242), originally published under the CC BY 4.0 license (https://creativecommons.org/licenses/by/4.0/). (c) Minimum energy paths for the double-kink nucleation, drawn with data from ref (242): enthalpy change, ΔH, as a function of both shear stress, τ, and reaction coordinate.