Bálint Korbuly1, Tamás Pusztai1, Hervé Henry2, Mathis Plapp2, Markus Apel3, László Gránásy1,4
1Institute for Solid State Physics and Optics, Wigner Research Centre for Physics, P.O. Box 49, Budapest H-1525, Hungary
2Laboratoire Physique de la Matière Condensée, École Polytechnique, CNRS, Université Paris-Saclay, 91128 Palaiseau Cedex, France
3Access e.V., Intzestr. 5, 52072 Aachen, Germany
4BCAST, Brunel University, Uxbridge, Middlesex, UB8 3PH, United Kingdom
In the literature, contradictory results have been published regarding the form of the limiting
(long-time) grain size distribution (LGSD) that characterizes the late stage grain coarsening in
two-dimensional and quasi-two-dimensional polycrystalline systems. While experiments and the
phase-field crystal (PFC) model (a simple dynamical density functional theory) indicate a lognormal
distribution, other works including theoretical studies based on conventional phase-field simulations
that rely on coarse grained fields, like the multi-phase-field (MPF) and orientation field (OF) models,
yield significantly different distributions. In a recent work, we have shown that the coarse grained
phase-field models (whether MPF or OF) yield very similar limiting size distributions that seem
to differ from the theoretical predictions. Herein, we revisit this problem, and demonstrate in the
case of OF models [by R. Kobayashi et al., Physica D 140, 141 (2000) and H. Henry et al. Phys.
Rev. B 86, 054117 (2012)] that an insufficient resolution of the small angle grain boundaries leads
to a lognormal distribution close to those seen in the experiments and the molecular scale PFC
simulations. Our work indicates, furthermore, that the LGSD is critically sensitive to the details of
the evaluation process, and raises the possibility that the differences among the LGSD results from
different sources may originate from differences in the detection of small angle grain boundaries.