In regard to thermodynamic stability of morphologies, molec-
ular assemblies are more stabilized in the order of sheet <
nanotube < vesicle under an assumption of the hydrophobic
edges of morphologies being the primary factor for destabili-
zation of the molecular assembly in water. Since the stability
of nanotube is just between vesicle and sheet, TEM observa-
tions of samples with varying duration of heat treatment were
examined to see whether nanotube morphology appears as a
transient morphology from sheet or micelle to vesicle upon heat
treatment. Interestingly, SLL-ECz took nanotube morphology
at 6 hours after heating as an intermediate morphology between
distorted sheet and vesicle (Figure S2). On the other hand,
neither SDL-NapIm nor SDL-Por took nanotube morphology
at any moment during the heating process. Taken together,
nanotube morphology to prepare from the helical polypeptides
specifically requires strict and tight helix association to cause
consecutive helix tilting in molecular assembly, which prevents
further conversion into vesicle upon heating. Previously, we
reported a similar observation with molecular assembly pre-
pared from (poly(sarcosine)) -b-(L-Leu-Aib) having the same
a)
b)
c)
Figure 4. a) Atomic force microscopy (AFM) in water
image and b) a height profile along the line in a) of molec-
ular assembly of a mixture of SLL and SDL. c) Schematic
illustration of the interdigitated monolayer of a mixture of
SLL and SDL.
2
6
helical hydrophobic block. This A B-type polypeptide took a
2
rolled-sheet morphology, which could not be converted even
into nanotube morphology upon heating.19 The tightness of
molecular packing should therefore decrease in the order of
SLL > SDL-ECz > SDL-NapImSDL-Por in light of the
most stable morphology.
Polydispersity indices of SDL-NapIm and SDL-Por vesi-
cles by DLS measurements were 0.64 and 0.82, respectively,
while a mixture of SLL and SDL (SLLSDL) and SLL-ECz
vesicles showed significantly smaller values of 0.19 and 0.1,
respectively, meaning that SDL-NapIm and SDL-Por gener-
ated vesicles of variable sizes. One reason for the polydisper-
sity may be the presence of tiny sheets or spherical micelles
prior to heating, which could fuse with each other to grow into
various sizes. On the other hand, SLL-ECz generated relatively
large distorted sheets of 100 nm size prior to heating, which
size may determine the following vesicle size upon heating.
by AFM in water, because the self-assemblies took distorted or
saddle-like sheet morphology. Vesicles are therefore subjected
to analysis by AFM in air to examine the membrane structure.
3.3 Dimensions of Peptide Vesicle by AFM in Air. AFM
images and mean heights of the four vesicles in air are sum-
marized in Figures 5 and 6. The SLLSDL vesicle shows an
average height of 13.0 nm, which is considered to be the sum of
two monolayers keeping the vesicle structure on the substrate
upon drying. The membrane thickness of one monolayer is
therefore 6.5 nm, which is a little bit less than 7.4 nm when
measured in water, probably because the hydrophilic layer was
dehydrated and became thinner. In the case of the SLL-ECz
vesicle, vesicles seemed to be ruptured on the APTES-modified
Si-wafer substrate to be transformed into a sheet shape, because
the observed height of 5.3 nm is close to the monolayer thick-
ness of the SLLSDL vesicle of 6.5 nm. On the other hand,
SDL-NapIm and SDL-Por showed average thicknesses of
20.2 nm and 18.7 nm, respectively, which seem that two mem-
branes should pile up because the vesicle structure was retained
on the substrate upon drying. The membrane thicknesses are
therefore 10.1 nm and 9.4 nm, respectively, which are still
thicker than the interdigitated monolayer of the SLLSDL
vesicle of 6.5 nm. 1,8-Naphthalimide and porphyrin chromo-
phores are large hydrophobic aromatics, and ππ stacking
interaction is also available to stabilize molecular associa-
3
.2 Dimensions of Peptide Sheet by AFM in Water.
Whether vesicle membranes take monolayer or bilayer struc-
ture, membrane thicknesses were evaluated by AFM in water
(Figure 4). The flat sheet of a mixture of SLL and SDL prior to
heating by TEM observation was observed similarly by AFM.
The average height of the flat sheet was found to be 7.4 « 0.79
nm. The molecular arrangement in the sheet is explained by
alternating SLL and SDL helices like a molecular checkerboard
pattern on the basis of electron diffraction pattern leading to
formation of interdigitated monolayer.12 The monolayer is thus
composed of two hydrophilic poly(sarcosine) layers flanking a
middle hydrophobic (Leu-Aib) layer (Figure 4c). Because the
6
2
0,21
helix length of the 12 residue is calculated to be 1.8 nm, one
poly(sarcosine) layer should be 2.8 nm thick on average. In the
interdigitated structure, a poly(sarcosine) chain at the N terminal
has a free space aside because the neighboring C terminals do
not have a poly(sarcosine) chain. Each poly(sarcosine) chain
tion.
Due to the large size of the chromophore, the critical
packing parameter of the amphiphilic molecules may change
the molecular shape relatively from a cone-shape to a cylin-
drical shape. SDL-NapIm and SDL-Por are therefore consid-
ered to take a bilayer structure, with which the membranes will
become thicker by the sum of one helix of 1.8 nm and aromatic
layer of 12 nm than the interdigitated monolayer. The ob-
served differences in thicknesses taking the SLLSDL mono-
layer as a reference are 3.4 nm and 2.9 nm, respectively for
SDL-NapIm and SDL-Por, which are thus in consistent with
(the most frequent residue numbers in the TOF Mass are 25 and
2
7 of SLL and SDL, respectively) therefore have a free space to
allow the chain taking a mushroom structure of 2.8 nm thick.
Unfortunately, other peptides of SDL-ECz, SDL-NapIm,
and SLL-Por could not be evaluated for membrane thickness
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