For direct tracking of individual particle motions with confocal laser microscopy, poly(methyl methacrylate) (PMMA) colloidal particles labeled with a fluorescent dye were used49 50 . As standard solvents for the colloidal droplets, a mixture of cis- and trans-decalin (Decahydronaphthalene, 99%, Sigma-Aldrich), were employed which has widely been used in drying experiments49 51 52 (link). Each droplet was gently deposited onto a clean cover glass (VWR, 22 × 30 mm2, No. 1.5) in all experiments. The initial drop volume was controlled to be V0 ≈ 0.5 μl, resulting in the initial contact radius of R0 ≈ 1.4 mm, which is smaller than the capillary length (≈1.9 mm for decalin): therefore, the droplet shape was assumed to be spherical. The PMMA colloids were prepared and supplied by A. Schofield (University of Edinburgh) according to the procedure described by Antl et al.53 , and thus were expected to show hard-sphere-like behaviors. The colloid radii were rS = 100 nm (small colloids) and rL = 1000 nm (large colloids) with ~5% polydispersity in size (previously determined by dynamic light scattering33 (link)). The density difference between colloids (1.19 g/cm3) and decalin (0.897 g/cm3) was small enough to prevent any sedimentation issues for the microscopic colloids54 .
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