Nanoparticle (NP) patterning on a
solid surface via nanofluid droplet
evaporation is one of the most fascinating topics of research. Quite
intriguingly, though a dose of excess ligand has been invariably included
in all of the experimental studies that resulted in large-area NP
patterns, the role of this excess ligand has been addressed inadequately
in the modeling studies carried out so far. Addressing this, we have
conducted systematic studies by including excess ligand both in our
experiments and modeling, and correlated the results with each other.
For this, we prepared nearly monodispersed thiol-protected gold nanoparticle
dispersion in toluene and added calculated amounts of excess thiol
before drop-casting it onto a transmission electron microscopy (TEM)
grid. Subsequently, upon solvent evaporation, the patterns formed
were imaged using conventional electron microscopy and analyzed with
customized image processing tools, to perform statistically significant
measurements. Our study demonstrates the ability of soluble excess
ligand to induce NP aggregation under nonequilibrium condition, leading
to large-area monolayer formation. These experimental results were
then rationalized by Monte Carlo simulations, based on a modified
coarse-grained two-dimensional (2D) lattice-gas model. We found that
excess ligand facilitates NP spinodal phase separation under nonequilibrium
conditions, largely governed by the interplay between ligand–solvent
and nanoparticle–ligand interactions. Using power spectrum
density analysis, we clearly demonstrate that these spatial patterns
have fractal surface characteristics due to persistent fractional
Brownian motion within subdiffusion limit.