T. Suzuki et al.
À
C
site sense of helicity, they were treated as single entities due
to facile interconversion.
equivalents of (4-BrC6H4)3N+ SbCl6 , the corresponding di-
À
cation salts 2a2+–d2+
[SbCl6 ]2 were isolated as deep purple
Upon recrystallization, a single-crystal specimen of 1c
(P212121, Z=8, two independent molecules) was obtained.
Interestingly, the crystal is composed of an equal amount of
diastereomers [(P)-1c for molecule-1, (M)-1c for molecule-
2], which is not a common crystallization phenomenon.[15a,b]
X-ray analysis provided structural information on both dia-
stereomers with the same point chiralities on the aryl rings,
but with a different helical sense (Figures 1c, d, and S3 in
the Supporting Information). Despite the similar helical ge-
ometries of the (P)- and (M)-isomers, their structural pa-
rameters differ slightly and indicate larger deformation in
crystals or amorphous compounds in high yields (93, 95, 98,
and 97%, respectively).[21] The salt of 2a2+ (see above) and
those of 2b2+–d2+ reproduced Ar4DMP 1a–d upon reduc-
tion with Zn dust in high yields (92, 95, 100, and 97%, re-
spectively), as was confirmed by the reversible nature of the
present redox pairs.
Interestingly, the reduction potentials of 2a2+–d2+ were
observed in the far cathodic region (Ered = +0.11, +0.07,
+0.03 and +0.03 V for 2a2+–d2+, respectively; two-electron
process). Such a large shift of redox peaks as well as a one-
wave two-electron oxidation process are commonly ob-
served in dynamic redox pairs[12] undergoing drastic structur-
À
the (M)-isomer. The torsion angle for the Ar2C=C C=CAr2
À
unit, the twisting angle of the biphenyl skeleton, and the
twisting angles of the two exocyclic bonds are 59.7(8),
23.1(9), 4(1), and 2(1)8 in the (P)-isomer and 69.4(6),
25.2(8), 10(1), and 8(1)8 in the (M)-isomer, respectively.
al changes and/or reversible formation/breaking of C C
bonds upon electron transfer.[7,8,14,22] The separation by ap-
proximately 0.6 V indicates a high electrochemical bistability
of the redox couples of 1/22+, which is favorable for re-
1
In the H NMR spectrum of 1c at room temperature, the
ACHTUNGTRENaNUGN lizing switching phenomena of redox active molecules.
À
only one set of resonances that correspond to a single C2-
symmetric species was observed, which shows that the two
diastereomers [(P)- and (M)-1c] exhibit indistinguishable
chemical shifts. The slightly different steric interactions for
the diastereomeric pair may or may not bias the equilibrium
ratio in favor of one of the two diastereomers,[20] however,
this issue cannot be detailed experimentally in either 1c or
1d for the same reason.
Upon crystallization of 2c2+
ACHTNGUTERUNN[G SbCl6 ]2 from CH2Cl2/ether,
a high-quality, single-crystal specimen was obtained, X-ray
analysis of which (P21, Z=2) revealed that the phenan-
threne core in 2c2+ is nearly planar (Figure 3). The two di-
AHCTUNGTREGaNNUN rylmethylium units are attached at the 9,10-positions with
large twisting angles [68(1) and 63(1)8] to give a helical ar-
rangement of the p system, the helical sense of which is sim-
ilar to that in (P)-1c. Although the helical inversion of (P)-
2c2+ can readily occur in solution through rotation about
+
the C9(10)
bonds, there are no diastereomeric dications
À
C
Redox properties and interconversion between Ar4DMPs
(1) and phenanthrene-9,10-diylbis(diarylmethylium)s (2):
Due to not only by the electron-donating alkoxy groups, but
also the observed skeletal deformation and intramolecular
p–p interaction, Ar4DMP 1a has an increased HOMO level,
so that it undergoes a facile electrochemical oxidation
(Eox = +0.61 V vs. Ag/Ag+ in CH2Cl2; two-electron pro-
with (M)-helicity in the crystal. Thus, the point chirality of
the alkoxy group [(R)-C2H5CHACHTNUGRTENUNG(CH3)O] is transmitted to the
(P)-helicity preference of the dication, in which the two
chromophores are stacked nearly in parallel with a shortest
À
C C contact of 3.05(1) ꢁ. Such an asymmetric geometry is
suitable for realizing exciton coupling of the two chromo-
À
G
phores.[23] Accordingly, the CD spectrum of 2c2+
N
A
salt, taken as a KBr tablet, showed the negative bisignated
Cotton effects in the l=500–600 nm region (Figure S4 in
the Supporting Information).
d, respectively; Figure 2). Upon treatment of 1a–d with two
Chiroptical properties and a multi-input/multi-output re-
sponse of 1c/2c2+ and 1d/2d2+: A large negative couplet
À
was observed in the CD spectrum of 2c2+
N
corded in CH2Cl2 [lext =591 nm (De=À23), 520 (+17)],
showing that the transmission of point chirality to helicity[15]
also occurs in solution to induce a preference for (P)-helici-
1
À
ty in 2c2+. In the H NMR spectrum of 2c2+
ACHTUNTRGENUNG[SbCl6 ]2, only
one set of resonances that corresponded to a single C2-sym-
metric species was observed, indicating that the two dia-
AHCTUNGTRENNUNG
stereomers [(P)- and (M)-2c2+] interconvert so rapidly that
we cannot determine the diastereomeric excess in terms of
the helicity preference. The observed ellipticity in 2c2+ is
much larger than that in the reference monocation [4-(R)-
À
C2H5CH
(CH3)O-C6H4]2CPh+BF4
[lext =508 (De=À1.3),
411 (À0.83), 270 nm (À1.4)],[15a] which can be explained by
the effective amplification of CD signals through exciton
coupling of the two cationic chromophores in the preferred
Figure 2. Cyclic voltammogram of 1c recorded in CH2Cl2 (0.5 mm) con-
taining Bu4NBF4 (0.1m) as a supporting electrolyte (E/V vs Ag/Ag+,
scan rate 100 mVsÀ1, Pt electrode).
120
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2013, 19, 117 – 123