Chemistry Letters Vol.38, No.9 (2009)
925
moieties. The dimethyl 2 had two Eoxs corresponding to the suc-
cessive generation of the radical cation and dication, as previ-
ously reported for long oligothiophenes.7 The cyclic voltammo-
gram of the diferrocenyl 1 revealed four reversible redox waves
(Figure 1a). The two lower waves were observed opposite each
other at 0.00 V, the Eox of ferrocene. In addition, the na up to the
second oxidation was 2.3 F molꢂ1 (two-electron oxidation).
These results indicate that the two lower redox waves at
Eoxs = ꢂ0:05 and 0.05 V and the two higher waves at
Eoxs = 0.26 and 0.58 V are assigned to the oxidation of the
two ferrocene moieties and the two stepwise oxidation of the
quaterthiophene moiety, respectively. For the monoferrocenyl
derivatives 3 and 4, three reversible redox waves were detected
(Figures S3 and S4)6 and the nas up to the first were 1.1–
1.2 F molꢂ1 (one-electron oxidation). These results suggest that
1.25
1.00
0.75
0.50
0.25
1.25
1.00
0.75
0.50
0.25
(a)
(b)
0
2
3
0
1
1
3
2
Energy/eV
Energy/eV
Figure 2. Electronic absorption of (a) 1 and (b) 2: neutral (solid
line) and one-electron oxidized (dashed line).
crease of the ꢀ–ꢀꢀ transition band, accompanied by the appear-
ance of two strong bands at 1.6 and 0.7 eV. This spectral change
during one-electron oxidation resembles those of 2 and previous-
ly reported oligothiophene derivatives,7 being interpreted as the
generation of a cation radical (polaron). These results evidenced
the presence of an oxidizing species such as a cation radical in
the quaterthiophene moiety of one-electron oxidized 1. There-
fore, the one-electron oxidizing species does not remain in the
one ferrocene moiety of 1, but spreads over the ferrocene and
the quaterthiophene moieties, and then would coulombically in-
teract with the other ferrocene moiety.
In summary, an unsymmetrically substituted quaterthio-
phene with two terminal ferrocene groups, 1, was prepared as
a long ꢀ-conjugated system with two redox active terminals.
The electrochemical and optical properties were compared with
those of a series of the quaterthiophene derivatives, 2–4. The re-
sults show that the one-electron oxidation of 1 would occur at the
ferrocene moiety attached to the end methoxythiophene ring and
the resulting oxidizing species extends to the neighboring qua-
terthiophene moiety. The extended oxidizing species would
electrostatically interact with the other terminal ferrocene moie-
ty. The present results demonstrate the effectiveness of substitu-
ents on the quaterthiophene moiety for controlling the oxidation
process in long conjugated systems having terminals.
the lowest redox waves (at Eox ¼ ꢂ0:05 V for
3 and
Eox ¼ ꢂ0:01 V for 4) and the two higher waves (at Eoxs =
0.14 and 0.54 V for 3, and Eoxs = 0.14 and 0.47 V for 4) are at-
tributed to the oxidation of the ferrocene moieties and the two
stepwise oxidation of the quaterthiophene moieties, respectively.
Figure 1b displays the square wave voltammograms of 1, 3,
and 4 in the voltage range from ꢂ0:20 to 0.15 V. The peak po-
tentials of the waves agreed within limits of error with the cor-
responding Eoxs obtained by CV. The waves attributable to the
oxidation of the ferrocene moieties in 3 and 4 were observed
at ꢂ0:05 and ꢂ0:01 V, respectively. Both the peak potentials
are shifted from the Eox of ferrocene, 0.00 V, and the degrees
of the shifts are apparently different. These results demonstrate
that the intensity of the interaction between the two neighboring
moieties, the ferrocene moiety and the quaterthiophene moiety,
would depend on the substituted position of the ferrocenyl group
on the unsymmetric quaterthiophene moiety; the ꢁ-position of
the end methoxythiophene ring for 3 and the ꢁ-position of the
end hexylthiophene ring for 4. The voltammogram of 1 shows
two waves at ꢂ0:05 and 0.05 V assignable to the oxidation of
the two ferrocene moieties. The peak potential of the one wave
(at ꢂ0:05 V) agrees with that of the wave due to the ferrocene
moiety in 3, however, the peak potential of the other (at
0.05 V) is clearly higher than that of the wave due to the ferro-
cene moiety in 4 (at ꢂ0:01 V). That is, the two peak potentials,
the Eoxs, of the ferrocene moieties in 1 are not completely con-
sistent with the combination of the peak potentials, the Eoxs, of
the ferrocene moieties in 3 and 4. The inconsistence of the poten-
tials leads us to infer that the two terminal ferrocenyl groups in 1
interact with each other. Further, the agreement of the first Eox of
the ferrocene moiety in 1 and the Eox of the ferrocene moiety in 3
implies that the one-electron oxidation of 1 occurs at the ferro-
cene moiety that is attached to ꢁ-position of the end methoxy-
thiophene ring and the interaction between the ferrocene moie-
ties in 1 does not take place in the neutral state but in one-elec-
tron oxidized state.
References and Notes
1
2
3
A.-C. Ribou, J.-P. Lanunay, M. L. Sachtleben, H. Li, C. W.
a) M. Iyoda, T. Kondo, T. Okabe, H. Matsuyama, S. Sasaki, Y.
W. Skibar, H. Kopaka, K. Wurst, C. Salzmann, K.-H. Ongania, F. F.
J. Casado, S. R. Gonzalez, M. C. R. Delgado, M. M. Oliva, J. T. L.
4
5
To elucidate the oxidized state of 1, a stoichiometric amount
of FeCl3 was added to a dichloromethane solution containing
2:0 ꢁ 10ꢂ3 M of each 1 and 2 and then the chemically oxidized
solutions were subjected to electronic absorption spectral analy-
sis. Figure 2 shows the spectra of 1 and 2 in neutral and one-elec-
tron oxidized states. The spectrum of neutral 1 has a ꢀ–ꢀꢀ tran-
sition band at 2.8 eV.
6
7
Supporting Information is available electronically on the CSJ-
Nakanishi, N. Sumi, S. Ueno, K. Takimiya, Y. Aso, T. Otsubo, K.
The one-electron oxidation of 1 resulted in a remarkable de-