“…Since the interface width W 0 = ξd 0 is adjusted by varying the numerical parameter ξ, this fixes the relaxation time to τ 0 = (47 √ 2/120)(d 2 0 /D)ξ 3 . In the present work, as in [4,19,22,23], the equation for the time evolution of the phase-field is written in terms of the anisotropy vector A. This vector appears when, in the original phase-field equation for solidification of a pure melt [21], one rewrites the following sum of three terms as a vector divergence, η=x,y,z…”