Phase-field models for strongly anisotropic surface energy need to be regularized to remove the ill posedness of the dynamic equations. Regularization introduces a new length scale, the corner size, also called the bending length. For large corner size, with respect to interface thickness, the phase-field method is known to converge asymptotically toward the sharp-interface theory when the appropriate approximation of the Willmore energy is used. In this work we study the opposite limit, i.e., corner size smaller than the interface width, and show that the shape of corners, at equilibrium, differs from the sharp-interface picture. However, we find that the phase transition at the interface is preserved and presents the same properties as the classical problem.