Dendrons of Amino Acids
this case, we presume that the
molecules are trapped in an
amorphous state, which might
be ascribed to the fast evapora-
tion of chloroform.
The solvents also played a
critical role in the self-assembly
of Nap-G2. The high solution
viscosity of Nap-G2 in acetone
and alcohols shall arise from
the long microbelts that inter-
cross each other. We found that
slow evaporation of the solvent
could lead the microbelts to
settle at the bottom of the cuv-
ette, thus forming a piece of dry
white sheet with the long axis
of microbelts parallel to the
sheet surface. The sheet could
be employed to run the
2D WAXD test in two orthogo-
nal directions (see the insets of
Figure 7a and b, wherein the
x direction is parallel to the
sheet surface and the z direc-
tion is the normal surface). Fig-
Scheme 1. Structures of Nap-G1 and Nap-G2. a) SOCl2, reflux, 2 h; b) CF3COO-G1, triethylamine, CHCl3, RT,
24 h; c) CF3COO-G2, triethylamine, CHCl3, RT, 24 h. For synthetic details, see the Supporting Information.
state. Hence, each lamella might consist of two layers of
Nap-G1, in which the naphthyl groups are partially interdi-
gitated with the benzyl groups. This packing fashion may
provide an additional driving force for the self-assembly of
Nap-G1.[20] Figure 5b depicts a schematic model of the mo-
lecular packing. As the lamellar period is smaller than twice
the extended molecular length of Nap-G1, interdigitated bi-
layers are easily formed through intermolecular hydrogen
bonding and p–p stacking interactions.
As shown in Figure 1, Nap-G1 xerogel obtained from the
mixed solvent of chloroform/petroleum ether (1:5, v/v) pres-
ents the spherulitic network, which is drastically different
from that of Nap-G1/cyclohexane. This implies that the mo-
lecular packing would also be different. The diffraction pat-
tern of Nap-G1/mixed-solvent xerogel exhibits a set of well-
resolved diffraction peaks (Figure 6), thereby indicating a
crystalline structure with an order higher than the lamellar
packing of Nap-G1 in cyclohexane. The first-order diffrac-
tion centered at 2q=3.48 corresponds to a d spacing of
2.6 nm, which is smaller than the layer period of the interdi-
gitated b-sheet structure but is still much larger than the
size of the Nap-G1 with an extended conformation. As the
WAXD powder pattern lacks dimensionality, the crystalline
structure cannot be solved at this moment. It is also intrigu-
ing to observe that the solvent with relatively high polarity
can completely inhibit the ordered packing of Nap-G1. In
Figure 6, the WAXD pattern from a powder sample ob-
tained after drying the Nap-G1/CHCl3 solution only shows
an amorphous halo in the low-angle region, the center (at
around 2q=5.88) of which corresponds to a dimension of
1.5 nm, which is close to the molecular size of Nap-G1. In
ure 7a and b depict the 2D WAXD patterns of a sheet
sample obtained from Nap-G2/acetone with the X-ray inci-
dent beam perpendicular and parallel to the z direction, re-
spectively. The ring pattern of Figure 7b indicates that the
ordered domains within the sheet are rotationally disor-
dered around the z direction. On the other hand, Figure 7a
reveals the orientation of the sample. On the basis of the
diffraction geometry, we assume that the diffraction arcs
along the z direction can be attributed to (hk0), whereas
those along the x direction are (00L). The detailed indices
of the integral-intensity profile of the 2D WAXD patterns
are shown in Figure 7c (see also Table S1 in the Supporting
Information). This indexing corresponds to an orthorhombic
cell with a=3.05 nm, b=2.66 nm, and c=0.83 nm. In this
case, it is very possible that the Nap-G2 molecules form col-
umns that pack parallel to form a 2D centered rectangular
structure. Previously,[15c] we have shown that a dendritic ge-
lator with an azo group at the focal point formed a similar
type of architecture, which has also been described by Jang
and Aida[25] and Percec[26] in their study on dendritic mole-
cules. The density of the Nap-G2 sample was measured to
be 1.30 gcmÀ3. With the value of the c axis of 0.83 nm, a cal-
culation based on the method by Percec et al.,[26] we deter-
mined that the number of the molecules located in each
column in the rectangular unit cell is 2.4. Figure 7d shows
the WAXD powder pattern of the Nap-G2/chloroform xero-
gel. It can be seen that some strong diffractions of the xero-
gel peak at similar positions appear in Figure 7c; however,
some diffractions (particularly those in the high-angle
region) are much broader, indicating that the packing of the
molecules are less perfect. Moreover, we can observe two
Chem. Asian J. 2011, 6, 1163 – 1170
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