Time-structuring in the evolution of 2D nanopatterns through interactions with substrate
Hydrophobic dodecanethiol capped gold nanoparticles (AuNPs) are found to self-assemble into two-dimensional patterns in monolayers of amphiphiles spread at the air-water interface of a Langmuir trough. In this communication we investigate the role of the nanoparticle-monolayer ( F NMA ) and monolaye...
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Veröffentlicht in: | Soft matter 2016-01, Vol.12 (27), p.5867-5875 |
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Zusammenfassung: | Hydrophobic dodecanethiol capped gold nanoparticles (AuNPs) are found to self-assemble into two-dimensional patterns in monolayers of amphiphiles spread at the air-water interface of a Langmuir trough. In this communication we investigate the role of the nanoparticle-monolayer (
F
NMA
) and monolayer-monolayer (
F
MMA
) lipophilic attraction in influencing morphology and dynamics of AuNP cluster patterns in fatty acid monolayers.
F
NMA
and
F
MMA
are progressively varied by changing
n
, where
n
is the number of -CH
2
groups in the alkyl tails of the amphiphilic fatty acid (CH
3
(CH
2
)
n
COOH) molecules forming the monolayer. Compressibility measurements on the pristine and nanoparticle-laden monolayers show that, while the compressibility of the pristine monolayer decreases with increasing
n
, pointing to a progressive increase in
F
MMA
, the effect of nanoparticles (increase in compressibility or lowering of
F
MMA
) is discernible only for 14 <
n
< 22. The corresponding pattern morphology, observed with a Brewster Angle Microscope (BAM) at an in-plane resolution of 450 nm for 6 hours, reveals that there are essentially three stages in pattern evolution, lamellae of Au nanoclusters spread over the fatty-acid monolayer background (the λ state) followed by a network of nanoclusters with high node density (the ν state) and finally rings (circular/elongated) of random sizes with very low node density (the ρ state), evolving from an initial unsegregated state, without appreciable change in the average nanoparticle number density over the field of view. Increasing
F
NMA
alongwith
F
MMA
is found to shift a certain state to later times, thus playing the role of a viscous drag and introducing a delay in the timeline. The mean square fluctuation of BAM intensity remains flat and then decays as
f
(
ξ
) =
ξ
2
H
over smaller length scales, where
ξ
is the spatial separation and
H
the Hurst exponent. The study of
f
(
ξ
) over time reveals the growth of a sub-diffusive regime (
H
< 0.5) at the intermediate length scale, in almost all the films coinciding with the emergence of the ρ state. The growth of this sub-diffusive regime is slower for stronger
F
NMA
and
F
MMA
, the interactions thus acting as control parameters in dictating the time structure of the spatio-temporal patterns.
Hydrophobic dodecanethiol capped gold nanoparticles (AuNPs) are found to self-assemble into two-dimensional patterns in monolayers of amphiphiles spread at the air-water interface of a Langmuir |
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ISSN: | 1744-683X 1744-6848 |
DOI: | 10.1039/c6sm00814c |