Fig. 2 | Nature Communications

Fig. 2

From: Tunable assembly of truncated nanocubes by evaporation-driven poor-solvent enrichment

Fig. 2

Assembly of mesocrystals grown at different VGS/VPS ratios by evaporation-driven poor solvent enrichment. a Left: optical image of the vessel after mesocrystal formation is complete (sample #1); the initial liquid level and the height for the onset and completion of mesocrystal growth are indicated as H(0), H(t1), and H(t2), respectively. Right: the VGS(t) (solid lines) and P(t) (dotted lines) curves for VGS/VPS = 2.5, NPE = 1 (black square), VGS/VPS = 5, NPE = 1 (red filled circle), VGS/VPS = 12.5, NPE = 1 (blue triangle), and VGS/VPS = ∞, NPE = 1 (purple diamond). The auxiliary lines and shaded regions show Δt and cC, estimated from the position of H(t1) and H(t2). Scanning electron microscopy (SEM) images for individual mesocrystals, high-resolution SEM (HRSEM) of the mesocrystal facets and corresponding fast-Fourier transform (FFT) patterns of mesocrystals grown from dispersions at VGS/VPS ratios of: b 2.5; c 5; d 12.5; e ∞. Scale bar = 10 μm for all SEM images and = 100 nm for all HRSEM images. f Apparent size of mesocrystals (filled symbols) and \(\frac{{c_{\mathrm{C}}}}{{\Delta t}}\) (open diamonds) as a function of VGS/(VGS + VPS). Error bars for the size represent the standard deviation of the mean (number of measurements: 290 for #1, 145 for #2, 118 for #3, and 306 for #4)

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