We have performed Monte Carlo simulations of hard spheres on a pattern under gravity. We found that a crystal formed at a moderate gravity strength contains essentially no defects while the one formed at a higher gravity strength contains a significant amount of defects. This result suggests the possibility of using gravitational tempering in a colloidal epitaxy to reduce the number of defects in the colloidal crystals. Moreover, we wish to emphasize on the possibility of obtaining a perfect crystal.Colloidal epitaxy was first proposed in 1997 by van Blaaderen et al.1 as a method to reduce stacking disorders in colloidal crystals. The basic idea of colloidal epitaxy is that the uniqueness of the stacking sequence for face-centered cubic (fcc) (001) stacking reduces the stacking disorders. Fcc (001) stacking was forced in a colloidal epitaxy by using a pattern on the substrate. Additionally, Zhu et al.2 in 1997 found that gravity reduces the stacking disorder in hard-sphere (HS) colloidal crystals. We have already found a glide mechanism for shrinking a stacking fault through a Shockley partial dislocation in fcc (001) stacking in HS crystals by Monte Carlo (MC) simulations.
3This mechanism has also been suggested by MC simulations of colloidal epitaxy on a square pattern under gravity. 4,5 In the present work, we study the possibility of gravity-induced tempering based on MC simulations. The number of defects is reduced with increasing gravity for a small range of gravity strength. But, it decreases with decreasing gravity in other ranges. In other words, the relationship between the number of defects and the strength of gravity is not monotonic; the amount of defects reaches a minimum at an optimum gravity strength. Similarly, up to a certain gravity strength, the crystallinity improves with the increasing gravity. In particular, no defects were observed in the bottom region at this gravity. We propose that settling a colloidal crystal at an optimum gravity strength reduces the number of defects. In other words, one can obtain a perfect crystal with the gravitational tempering.In 1957, the existence of a crystalline phase in an HS system was shown by MC 6 and molecular dynamics (MD) 7 simulations. In the HS system, the phase behavior is governed only by the particle number density. The fluid and the crystalline phases are separated by a coexistence region of 0.494 < º < 0.545 8 (In 1998, the coexistence densities were revised by Davidchack and Laird 9 as º f = 0.491 and º s = 0.542 by an MD simulation of a direct crystal-fluid coexistence). Here, º Ô (³/6)· 3 (N/V) is the volume fraction of the HSs with · being the HS diameter; N, the number of particles; and V, the volume of the system. As the density increases, the HS system crystallizes. Accordingly, the HS colloids, and also the charge-stabilized colloids with repulsive screened Coulombic interaction, crystallize by sedimentation.10 Defects contained in the colloidal crystals obtained without invention are, however, inevitable.In applications such as produc...