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These parameters have significant effects on the microstructure in terms of variance of the cluster height, width or size.
In this case, wedge-like huts have different ridge structures (the ridge width and location of atoms on it) depending on cluster height.
From the AFM images the Au NPs height distributions were determined by using a software (Nanoscope IIIa) that define each nanocluster area by the surface image sectioning of a plane that was positioned at half cluster height.
From the quantification of the time evolution of the mean cluster height, a time exponent 1/z = 0.54 ± 0.04 was evaluated, indicating a three-dimensional cluster growth in which the full clusters surface is active in the mass transport.
The AFM analyses allowed to study the evolution of the mean cluster height as a function of annealing time for each fixed temperature, showing a power-law behavior characterized by a temporal exponent whose value suggest that the full cluster surface is active in mass transport.
P-value was calculated by counting the frequency of maximum cluster height from the 500 repeats.
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In this scenario, the structures of both apexes of huts are independent of cluster heights, that agrees with experimental observations.
Experimentally, Cs atom nucleation at defect sites seems to culminate at Cs cluster heights near 1 nm and cluster diameters near 5 nm.
The ridge structures of the 2-ML and 6-ML wedges are seen to coincide, which is not the case for different cluster heights.
A complete set of the wedge ridges for different cluster heights can be obtained by filling the terraces by epi-oriented pairs of dimers.
The p-cluster height h obtained by this way is in a good agreement with its determination by AFM technique (see Fig. 3).
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com