317
R2
8
7
6
5
Br
R2
a
Br
Br
4
3
R2
Br
2
1
0
2a: R2
2b: R2
=
=
(95%)
(93%)
R2
500
250
300
350
400
450
Wavelength / nm
b, d
66% (2 steps)
c, d
2a
1-C3
2b
1-C1
88% (2 steps)
Figure 3. Dependence of the absorption coefficients for 1-U3-F
(white circles), 1-C3-F (gray circles), 1-C1-F (black circles),
and TPPy-F (solid line) on the wavelength. The absorption
coefficients were obtained by normalizing the absorbance of the
films at every wavelength according to the film thicknesses.
Scheme 1. Synthetic routes to newly designed TPPy-bridged
alkoxysilane precursors; 1-C3 and 1-C1. Reagents and con-
ditions: (a) [Pd(PPh3)4], K2CO3 (aq), 4-allylphenylboronic acid,
1,4-dioxane, 90 °C for 2a, [Pd(PPh3)4], K3PO4 (aq), 4-vinyl-
phenylboronic acid, 1,4-dioxane, 80 °C for 2b; (b) H2[PtCl6]¢
6H2O, HSiCl3, benzene, 40 °C; (c) [PdCl(³-C3H5)]2, rac-H-
MOP, HSiCl3, benzene, 40 °C; (d) i-PrOH, pyridine, CH2Cl2,
0 °C-rt.
to the suppression of heterogeneous shrinkage during solvent
evaporation.16 The thicknesses of 1-U3-F, 1-C3-F, and 1-C1-F
were 1450 « 50, 455 « 30, and 235 « 30 nm, respectively. The
change in the thickness can be attributed to the difference in the
viscosity of the sol solutions.
To overcome these limitations and difficulties, we employed a
useful approach, the Suzuki-Miyaura coupling of aryl halide with
olefin-substituted phenylboronic acid as shown in Scheme 1.14
The olefinic TPPy derivatives 2a and 2b were synthesized
by the palladium-catalyzed Suzuki-Miyaura coupling of 1,3,6,8-
tetrabromopyrene with 4-allylphenylboronic acid or 4-vinyl-
phenylboronic acid, respectively (Scheme 1). Each reaction
successfully proceeded in the presence of [Pd(PPh3)4] (12
mol %) as catalyst and gave the desired product 2a and 2b in
95% and 93% yield, respectively. Fortunately, undesired side
reactions such as isomerization and polymerization of olefinic
moiety were not observed. The obtained 2a and 2b were then
regioselectively hydrosilylated with trichlorosilane in the pres-
ence of platinum or palladium catalyst, respectively. The use of
H2[PtCl6]¢6H2O (Speier’s catalyst)11 was found to be effective
for 2a. The hydrosilylation proceeded regioselectively at £-
position of four allyl groups and gave the TPPy-bridged
trichlorosilane in almost quantitative yield. The 4-fold hydro-
silylation of 2b was carried out in the presence of [PdCl(³-
C3H5)]2/rac-H-MOP.12 As expected, the reaction regioselective-
ly proceeded at ¡-positions of four vinyl groups and furnished
the desired TPPy-bridged trichlorosilane quantitatively. How-
ever, the obtained chlorosilanes were too moisture-sensitive to
handle as a precursor for the organosilica hybrids. Thus, these
trichlorosilyl groups were transformed into relatively stable
triisopropoxysilyl groups by quenching with 2-propanol in the
presence of pyridine as a base, which afforded desired TPPy-
bridged alkoxysilane precursors with short linkers 1-C3 and
1-C1 in 66% and 88% yield, respectively (Figures S1-S4).15,18
From TPPy-bridged organosilanes 1-U3, 1-C3, and 1-C1,
organosilica hybrid films could be obtained by sol-gel polymer-
ization in the presence of hydrochloric acid and water in
propylene glycol propyl ether. Transparent yellow films without
cracks and inclusions were successfully obtained from all the
precursors (Figure S518). The use of the high boiling point
solvent facilitates the formation of uniform thickness of film due
We evaluated the optical properties of TPPy-bridged
alkoxysilane precursors and derived organosilica films to
elucidate the effects of the linker length on accumulation state
of TPPy moieties in these silica hybrids. The novel TPPy
precursors 1-C3 and 1-C1 showed primary similar absorption
and fluorescence properties compared with those of conventional
precursor 1-U3 and their parent TPPy molecule (Figure S618).
This suggests that the present linkers hardly influenced the
electronic ground and excited state of these precursors in diluted
condition. In contrast, optical properties of derived organosilica
films were quite different from one another. Figure 3 shows the
wavelength dependence of the absorption coefficients (absorb-
ance normalized by the film thickness) for organosilica and
TPPy molecular films (TPPy-F). The absorption coefficient was
significantly increased in the order of 1-U3-F (17000 cm¹1) <
1-C3-F
(29400 cm¹1) < 1-C1-F
(39900 cm¹1) < TPPy-F
(59800 cm¹1). It is quite reasonable to observe the difference
in absorption coefficients because the ratios of TPPy moiety to
whole molecules are completely different in their precursors.
The maximum wavelengths of absorption spectra (-max) slightly
red-shifted with respected to that for corresponding precursor
solutions due to intermolecular interaction between TPPy
moieties at the ground state. However, the observed red shift
in the films is very small and shift values do not depend on the
linker length. This may be attributed to the bulky structure of
TPPy which inhibits dense packing of TPPy moiety in organo-
silica hybrids.
Figure 4 shows fluorescence emission spectra for the
organosilica and TPPy molecular films. The organosilica film
1-U3-F showed broad emission bands at 450 and 470 nm which
are assignable to monomer-like and excimer emissions, respec-
tively.9 The existence of the strong monomer-like band and the
relatively small red shift of the excimer band suggest relatively
weak intermolecular interaction between the TPPy moieties
in the excited state due to the long linker length in 1-U3. In
Chem. Lett. 2012, 41, 316-318
© 2012 The Chemical Society of Japan