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n carbon number in the spacer moiety, however, the transparent gels could not be obtained even in the presence of [60]fullerene. Further investigation of the gellike aggregates has not yet been carried out.
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θ=0 (433 nm) did not coincide with the Soret absorption band at 441 nm.
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Secondary interaction between two neighboring porphyrins in different fibers would be possible to stabilize the gel structure even in the absence of [60]fullerene, and it seems to be reflected by the complicated CD pattern in Figure 4b. However, such a secondary interaction occurs mainly at the junction points to form aggregates of one-dimensional fibers. It is expected that the population of the secondary interaction is much smaller than that of the main porphyrin-porphyrin interaction in the one-dimensional fibers. We concluded that the complicated CD pattern in Figure 4b is mainly ascribed to the less ordered gel structure of 5a in the absence of [60]fullerene.
-
-
-
-
54
-
-
0011297627
-
-
note
-
The detection of the C=O stretching bands was very difficult due to the overlap with the solvent toluene bands.
-
-
-
-
55
-
-
0011300717
-
-
note
-
Table 2 indicates that 5c in the absence of [60]fullerene could not gelate benzene at 5 °C. This is attributed to cryoscopy induced by the gelator.
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0009312119
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Now it is not clear whether the twisted aggregate structure found in the SEM picture (Figure 7b) can be ascribed to the helical structure of the one-dimensional fiber and/or the chiral aggregate mode of the small fibers. Monitoring the gel formation by AFM (ref 24) and by synchroton small-angle X-ray scattering (e.g.: Sakurai, K.; Oho, Y.; Jung, J.H.; Okamoto, S.; Sakurai, S.; Shinkai, S. J. Chem. Soc., Perkin Trans. 2 2001, 108-112) would be effective methods to check the nature of the twisted structure. However, those measurements were difficult due to the stability problem of the gel.
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Sakurai, K.1
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0011345076
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note
-
In the cases of metalloporphyrin systems, van der Waals interaction, charge-transfer interaction between porphyrin and fullerene systems, and metal-ligand-type interaction between central metal atom and fullerene π system have been proposed by several groups as main forces of interaction (see ref 15). In the 5/[60]fullerene system, Zn(II)-ligand-type interaction would play an important role along with van der Waals interaction and charge-transfer interaction, because the free porphyrin appended gelator 4 did not form a stable gel in the presence of [60]fullerene. However, it is difficult to say which type of interaction is the main force here.
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