Hetero-Double-Helix Formation by an Ethynylhelicene Oligomer
FIGURE 6. Proposed effect of hard arenes arranged among soft arenes
in (P)-6.
FIGURE 9. CD spectra of a 1:1 mixture of (P)-1 and (P)-6 (trifluo-
romethylbenzene, total concentration 2.5 × 10-5 M, 5 °C), (P)-1, and
(P)-6 (trifluoromethylbenzene, 1.25 × 10-5 M, 5 °C) obtained within
30 min of cooling. The spectrum calculated by adding those of (P)-1
and (P)-6 is also shown.
Since a new double-helix-forming (P)-6 possessing perfluo-
rooctyl side chains was obtained in this study, the interactions
between (P)-6 and the conventional oligomer (P)-1 were
examined. Experiments were conducted to determine whether
(P)-1 and (P)-6 form heterodimers or a mixture of individual
homodimers. It was also of interest to compare the interactions
of (M)-1 and (P)-6 to examine the chiral recognition phenomena.
Our previous studies revealed that the same configurations were
favored as for the enantiomeric helicenes in noncovalent
interactions.16
FIGURE 7. CD spectra (toluene, 5 °C) of (P)-1 (5 × 10-5 M and 1 ×
10-4 M) and (P)-6 (5 × 10-5 M).
The complexation of (P)-1 and (P)-6 was examined in
trifluoromethylbenzene, in which the total concentration of (P)-1
and (P)-6 was adjusted to 2.5 × 10-5 M, because both formed
a double-helix at 1.25 × 10-5 M at 5 °C (Figure 9). Solutions
of (P)-1 and (P)-6 in trifluoromethylbenzene were prepared and
were mixed in a 1:1 ratio at room temperature. The solution
was then cooled to 5 °C, and the CD spectra were obtained
within 30 min. The 1:1 mixture showed a spectrum similar to
the sum of the spectra10 of each double-helix in trifluorometh-
ylbenzene (1.25 × 10-5 M, 5 °C), which suggested the
formation of homo-double-helices (Figure 9). In order to further
confirm this interpretation, the ratio of (P)-1 to (P)-6 was
changed, keeping the total concentration at 2.5 × 10-5M (Figure
10a), and ∆ꢀ value at 330 and 370 nm were plotted against the
ratio of (P)-1 to (P)-6 (Figure 10b). Both plots were on
approximate straight lines giving the maxima of the ∆ꢀ value
for pure (P)-1 and pure (P)-6. It was therefore concluded that
the structural changes of (P)-1 and (P)-6 were independent and
resulted in the formation of individual homo-double-helices.
CDs were measured in a solvent of less helix-forming
tendency. In toluene (1 × 10-4 M, 5 °C), (P)-6 formed a partial
double-helix, and (P)-1 was random coil. The 1:1 mixture of
(P)-1 and (P)-6 showed a spectrum similar to the sum of both
FIGURE 8. CD spectra (m-difluorobenzene, 1 × 10-4 M) of (P)-1 (5
and 60 °C) and (P)-6 (5 °C).
chain to the S-side chain14 or by external stimuli such as changes
in pH, solvent, and temperature.15 The inversion of a double-
helix depending on solvent has been also reported.5d These
observations of (P)-6 and (P)-1 are another notable example of
such inversions caused by the effect of achiral side chains.
The stability of the double-helix structure was compared
between (P)-6 and (P)-1. In toluene, (P)-6 showed an increase
in |∆ꢀ| compared to the random coil state at 5 × 10-5 M, while
(P)-1 was in the random coil state even at 1 × 10-4 M (Figure
7). In m-difluorobenzene at 1 × 10-4 M, (P)-6 showed a
spectrum with relatively increased |∆ꢀ| over the random coil
state due to a partial double-helix structure, and (P)-1 was
random coil (Figure 8). In general, (P)-6 formed a double-helix
at lower concentrations than (P)-1, indicating that the double-
helix of (P)-6 is more stable than that of (P)-1. It was presumed
that the hard/hard π-π interactions strengthened the binding
and stabilized the double-helix structure of (P)-6, which
possessed alternating soft and hard arene moieties (Figure 6).
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