Crystals are known to grow nonclassically
or via four
classical
modes (the layer-by-layer, dislocation-driven, dendritic, and normal
modes, which generally involve minimal interfacet surface diffusion).
The field of nanoscience considers this framework to interpret how
nanocrystals grow; yet, the growth of many anisotropic nanocrystals
remains enigmatic, suggesting that the framework may be incomplete.
Here, we study the solution-phase growth of pentatwinned Au nanorods
without Br, Ag, or surfactants. Lower supersaturation conditions favored
anisotropic growth, which appeared at variance with the known modes.
Temporal electron microscopy revealed kinetically limited adatom funneling,
as adatoms diffused asymmetrically along the vicinal facets (situated
inbetween the {100} side-facets and {111} end-facets) of our nanorods.
These vicinal facets were perpetuated throughout the synthesis and,
especially at lower supersaturation, facilitated {100}-to-vicinal-to-{111}
adatom diffusion. We derived a growth model from classical theory
in view of our findings, which showed that our experimental growth
kinetics were consistent with nanorods growing via two modes simultaneously:
radial growth occurred via the layer-by-layer mode on {100} side-facets,
whereas the asymmetric interfacet diffusion of adatoms to {111} end-facets
mediated longitudinal growth. Thus, shape anisotropy was not driven
by modulating the relative rates of monomer deposition on different
facets, as conventionally thought, but rather by modulating the relative
rates of monomer integration via interfacet diffusion. This work shows
how controlling supersaturation, a thermodynamic parameter, can uncover
distinct kinetic phenomena on nanocrystals, such as asymmetric interfacet
surface diffusion and a fundamental growth mode for which monomer
deposition and integration occur on different facets.