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10.1002/chem.202102421
Chemistry - A European Journal
FULL PAPER
DMSO solution with fluorescence quantum yields of 17 % and
18 % for 1 and 2, respectively (Figure 1b and Figure S1). These
results imply that 1 and 2 exist as monomeric species in DMSO
and undergoes amphiphilicity-driven self-assembly with the
addition of water into their DMSO solution mainly through p-p
stacking of the HPB units. The nearly non-emissive nature of the
monomeric species is due to the intramolecular C(sp2)-C(sp2)
bond rotational relaxation of the excited states of 1 and 2.
Whereas the intramolecular bond rotation is completely arrested
in the aggregated state, which facilitate the radiative decay
channel (fluorescence) of the excited states and thereby
enhances the emission in the aggregated state. This
phenomenon is known as aggregation induced enhanced
emission (AIEE) and is very typical of HPB-based systems.[17]
Temperature-dependent emission studies of the aggregates of 1
(Figure 1c) and 2 (Figure S2) in water:DMSO showed a decrease
in emission intensity with the increase in temperature from 20 °C
to 90 °C, and become almost non-emissive at high temperature.
Moreover, emission intensity of 1 in water:DMSO (aggregated
species) at 90 °C is nearly matching with the emission intensity of
1 in DMSO at 20 °C (monomeric species) (Figure 1c inset). These
results confirm that the amphiphiles exist as aggregated species
in water:DMSO at 20 °C and gradually breaks into the
corresponding monomeric species upon rise in temperature. It is
also to be noted a decrease in emission intensity of 1 in DMSO at
90 °C when compared to its emission intensity at 20 °C and this
can be attributed to the mere effect of temperature on
fluorescence (Figure 1c inset).[18] In support of this, dynamic light
scattering (DLS) analyses of 1 and 2 solution in water:DMSO
revealed the formation of aggregates with size distributions in the
ranges of 250 nm-5 µm and 50 nm-6 µm for 1 and 2, respectively
(Figure 1d).
Detailed microscopic analyses were then carried out to
understand the morphology of the aggregated species of 1 and 2.
Atomic force microscopic (AFM) analyses of the aggregates of 1
(Figure 2a) and 2 showed the formation of nanosheets with lateral
dimensions in the range of several micrometers. Section analyses
revealed that height of sheets of 1 is in the range of 20-100 nm
(Figure 2a inset). Height of the sheet is significantly larger than
the corresponding monolayer distance of 1 sheet (~5 nm),
suggesting that the sheets are multilayered in nature. Scanning
electron microscopic analyses of the aggregates of 1 (Figure 2b)
and 2 (Figure S4) also showed the formation of multilayered
sheets with lateral dimensions of several micrometers, which is in
good agreement with the AFM analyses. Sheet morphology was
further supported by transmission electron microscopic (TEM)
analyses, which revealed the formation of highly transparent
nanosheets for 1 (Figure 2c) and 2 (Figure S6). Furthermore, TEM
analyses clearly disclosed the multilayered nature of the sheets
(Figure 2d). All these results collectively conclude that both the
amphiphiles undergo amphiphilicity-driven self-assembly mainly
through p-p stacking interaction of HPB to micrometer-sized
b)
a)
500 nm
1 µm
d)
c)
multi layer
Figure 2. (a) AFM height, (b) SEM and (c) & (d) TEM images of 1 aggregates
in water:DMSO (98:2). Inset of (a) shows the section analysis of the sheet along
the line drawn on the image. [1] = 2 μM for all the experiments.
Synthesis of AgNPs and their immobilization onto the sheet
The most noteworthy structural feature of the sheets is the
extremely dense display of reducing sugar on the surface of the
sheets, which means that they offer a unique opportunity for the
in-situ synthesis of AgNPs by using the well-known Tollens’
reaction. Tollens’ reaction involves the reduction of Ag(1) to Ag(0)
by a reducing sugar such as galactose, which on the other hand
undergoes oxidation of the aldehyde group to the corresponding
carboxylic acid group. Subsequently, Ag(0) is acting as the seed
for the growth of NPs of defined size and shape. For this purpose,
Tollens’ reagent ([Ag(NH3)2]+) (20 mM) was added to the sheets
of 1 or 2 (20 μM) in water:DMSO (98:2), vortexed for 2 h in dark.
The in-situ formation of AgNPs was then followed by monitoring
the emergence of surface plasmon absorption band of the NPs at
400 nm. Interestingly, UV-visible absorption spectrum of the
solution of 1 sheet after 2h of reaction disclosed a strong
absorption band with maximum centered at 400 nm, which clearly
implies the in-situ formation of AgNPs (Figure 3a). In support of
this, the colorless reaction mixture turned into pale yellow (Figure
3b). Furthermore, a significant quenching of fluorescence was
observed for the sheets due to the electronic interaction between
AgNPs formed on the sheet and HPB (Figure 3c), which is very
much feasible as the distance separating them is only ~2.5 nm.
Similar observations were seen for 2 sheets as well (Figure S7–
S9).
multilayered sheets. Accordingly, sheet of 1, which is
a
bolaamphiphile, consists of monolayer assembly of 1 having p-
stacked HPB as the hydrophobic core with hydrophilic galactose
protruding on both the faces of the sheet as shown in Scheme 1.
Similarly, sheet of 2, which is an amphiphile, consist of bilayer
assembly of HPB through p-p stacking as the hydrophobic core
with hydrophilic galactose protruding on the faces of the sheet
(Scheme 1).
To gain better insights into the structural characteristics of
the NPs, detailed TEM analyses were carried out on the NPs
obtained after the reactions of 1 and 2 sheets with Tollens’
reagent. The TEM images of NPs in the case of 1 sheet revealed
that the NPs are spherical in shape and nearly monodisperse
(Figure 3d). The size of the NPs is in the range of 5-10 nm, which
falls in the regime of ultrafine NPs (Figure 3d inset).[19] It is also
obvious from the TEM images that the NPs are well-dispersed
3
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