lowed by a Sonogashira5,11 coupling with (trimethylsilyl)-
acetylene afforded the silylated oligomer 3. Protodesilylation
with potassium carbonate gave the acetylide arm 4 in
quantitative yield. To force complete substitution of the
appropriate aromatic halide, 9, 20, and 36 molar equiv of 4
were added to produce 5, 6, and 7, respectively, using
Sonogashira coupling.
The electronic spectra of the arm and radial homologues
were recorded in dichloromethane (Table 1); spectra of the
benzene-core series are shown in Figure 1. The absorption
Figure 2. Electronic absorption spectrum (-) and emission
spectrum (‚‚‚) for thin films of 7.
series for the solid and solution spectra. The series shows
surprisingly good linearity. Typically, a plot of ∆E vs 1/n
results in a linear relationship for π-conjugated oligomers
and a saturation limit for ∆E vs n is reached for a given
oligomer length.15 Clearly, this series of homologues is
unique as no hint of a saturation limit for ∆E is evident as
the number of thiophene rings is increased. To our knowl-
edge, such a relationship is unprecedented in thiophene-based
conjugated oligomers.
Figure 1. Electronic absorption spectra recorded in dichlo-
romethane for 4 (-), 5 (---), 6 (‚‚‚), and 7 ()).
maximum (λmax) for the lowest π-π* transition increases
with the number of arms around the benzene core. The trend
is consistent with a previously reported series of phenyl-
ethynyl-substituted benzene systems12 and is evidence of
extended π-conjugation through the benzene core. Homo-
logue 8 with the thiophene core exhibits a maximum
absorption at 402 nm and is substantially red-shifted relative
to the arm (374 nm), again suggesting the formation of a
delocalized π-system through the core.
Solid-state spectra of the homologues were also recorded.
Figure 2 shows the electronic absorption spectrum of a thin
film of 7 cast from a dichloromethane solution onto a cubic
zirconia ATR crystal. The spectrum is red-shifted compared
with the solution phase and exhibits low energy fine structure.
Both qualities are characteristic of solid-state spectra of
conjugated homologues and polymers.13 The large red-shift
has generally been attributed to enhanced planarity of the
molecule in the solid state. However, the origin of the fine
structure is still debatable and will not be discussed here.
Figure 3 shows plots of the lowest energy transition vs
the number of thiophene rings for the arm and benzene-core
Figure 3. Energy (∆E) of the lowest electronic transition for
solution (b) and solid (O) for 4-7 vs the number of thiophene
rings in the conjugated homologue.
The emissive properties of the homologues were also
studied in solution and in the solid state (Table 1, Figures 2
and 4). As in the case for the absorption spectra, the emission
spectra of the homologues display a distinct red-shift as the
number of thiophene rings increases. The radial homologues
exhibit good quantum efficiencies (g20%) in dichloro-
methane solution at room temperature (relative to the [Ru-
(10) (a) Cherioux, F.; Guyard, L. AdV. Func. Mater. 2001, 11, 305-
309. (b) Cherioux, F.; Maillotte, H.; Audebert, P.; Zyss, J. Chem. Commun.
1999, 2083-2084. (c) Cherioux, F.; Guyard, L.; Audebert, P. Chem.
Commun. 1998, 2225-2226.
(11) (a) Sonogashira, K.; Tohda, Y.; Hagihara, N. Tetrahedron Lett. 1975,
4467. (b) Takahashi, S.; Hagihara, N.; Kuroyama, Y.; Sonogashira, K.
Synthesis 1980, 627.
(14) Caspar, J. V.; Meyer, T. J. J. Am. Chem. Soc. 1983, 105, 5583-
5590.
(12) Kondo, K.; Yasuda, S.; Tohoru, S.; Miya, M. J. Chem. Soc., Chem.
Commun. 1995, 55-56.
(13) For example, see the following and references therein: Koren, A.
B.; Curtis, M. D.; Kampf, J. W. Chem. Mater. 2000, 12, 1519-1522.
(15) (a) Jestin, I.; Frere, P.; Mercier, N.; Levillain, E.; Stievenard, D.;
Roncali, J. J. Am. Chem. Soc. 1998, 120, 8150-8158. (b) Guay, J.; Kasai,
P.; Diaz, A.; Wu, R.; Tour, J. M.; Dao, L. H. Chem. Mater. 1992, 4, 1097-
1105.
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