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T. Amaya et al. / Tetrahedron Letters 51 (2010) 2416–2419
Figure 3. Synthesis of NPs-1 and its TEM image.
the solution of TPP, the decreasing of emission intensity was ob-
served with the increasing of the concentration of the aniline
chain. Stern–Volmer plot gave a linear relationship, and the
Stern–Volmer constant was 1.6 ꢁ 103 Mꢂ1 (Fig. S5). Concerning
about the Zn(II)-complexes Zn-1, Zn-2, and Zn-4 bearing the ani-
line chain, their emission intensity was also smaller than that of
Zn-TPP. Zn-1 and Zn-2 showed the larger emission than Zn-4,
where the coordination from the pyridyl moiety to the Zn(II) center
is likely to contribute.
Figure 2. (a) UV–vis absorption spectra of Soret and Q band region for Zn-1, Zn-2,
Zn-4, and Zn-TPP. (b) Emission spectra of 1, 2, TPP, Zn-1, Zn-2, Zn-4, and Zn-TPP
with excitation of the Qy(1,0) or Q(1,0) band for the free base porphyrins or Zn-
porphyrins, respectively. 5.0 ꢁ 10ꢂ6 M solution of CH2Cl2/THF = 995:5 under argon
atmosphere.
absorption spectroscopy. Measurement was carried out in the
5.0 ꢁ 10ꢂ6 M solution of CH2Cl2/THF = 995:5 under argon atmo-
sphere.8 Porphyrins bearing an aniline chain showed a broad
absorption around 280–350 nm derived from the aniline chain as
well as the characteristic Soret and Q bands (Fig. S3). Red-shift of
Soret and Q bands was observed with the Zn complex, Zn-1 and
Zn-2, as compared with Zn-TPP, however, the smaller shift was
observed with the Zn-4 complex which does not have a pyridyl
moiety (Figs. 2a and S4). The coordination of the pyridyl group to
the Zn-porphyrin is likely to contribute to the red-shift. Thus, the
self-assembly of the porphyrin bearing an aniline chain was
suggested.
Fluorescence emission spectroscopy with excitation of the
Qy(1,0) or Q(1,0) band was studied with 1, 2, TPP, and their Zn(II)
complexes, Zn-1, Zn-2, Zn-4, and Zn-TPP (Fig. 2b).9 Measurement
was also carried out in the 5.0 ꢁ 10ꢂ6 M solution of CH2Cl2/
THF = 995:5 under argon atmosphere. Significant quenching was
observed with 1 and 2 bearing the aniline chain, as compared with
that of TPP. It is likely due to the intramolecular photo-induced
electron transfer. This phenomenon was also consistent with our
previous reports.4 When the model aniline chain was added to
First oxidation and reduction potentials were obtained from the
differential pulse voltammograms of 1, 2, 7, TPP, and their Zn com-
plexes Zn-1, Zn-2, and Zn-TPP (Fig. S6). Measurement was carried
out in their 0.25 mM THF solution with Bu4NClO4 as an electrolyte
under argon atmosphere. Table 2 shows the potentials versus Fc/Fþ
c
and the driving force of photo-induced charge separation
DGCS
estimated by the equation:
D
GCS = E(DÅ+/D) ꢂ E(A/AÅꢂ) ꢂ E00, where
E00 is the energy of photoexcitation. First oxidation potentials are
approximately ꢂ0.14 V for 1, 2, Zn-1, Zn-2, and 7, assigned to
the one-electron oxidation of the aniline chain. On the other hand,
first reduction potentials are approximately ꢂ1.7 V for free base
porphyrins 1, 2, and TPP, and ꢂ1.9 V for Zn(II)-complexes Zn-1,
Zn-2, and Zn-TPP. Negative
DGCS was observed with 1, 2, Zn-1,
and Zn-2, which supports the results of decreasing of the emission
and suggests the intramolecular electron transfer.
Pyridyl group is known to act as a protecting group for Au nano-
particles.10 So, Au nanoparticles NPs-1 were synthesized by the
reduction of Na(AuCl4) using NaBH4 in the presence of the porphy-
rin 1. Its transmission electron microscopy (TEM) image is shown
in Figure 3. The average diameter is 3.0 nm and the particles are
independent. 1H NMR showed the presence of the porphyrins
without decomposition. There is no doubt that the porphyrins
act as a protecting group for the Au nanoparticles although direct
evidence was not obtained for the coordination of the pyridyl
group to the Au nanoparticles.
In summary, synthesis and Zn(II)-induced self-assembly of 1
and 2 were demonstrated. Au nanoparticles protected with 1 were
also synthesized. They are of potential use in a variety of applica-
tions such as redox-active receptors and photo-active catalysts or
materials. Further investigation is now in progress.
Table 2
The redox potential (V vs Fc/Fþc ) and driving force of the photo-induced charge
separation
DGCS (V) for 1, 2, TPP, Zn-1, Zn-2, Zn-TPP, and 7 (0.25 mM in THF
containing 0.1 M Bu4NClO4)
a
Redox potential (V vs Fc/Fcþ
)
D
GCS (V)
E(Por/PorÅꢂ
)
E(DÅ+/D)
1
2
ꢂ1.68
ꢂ0.14
ꢂ0.14
+0.60
ꢂ0.14
ꢂ0.15
+0.40
ꢂ0.14
ꢂ0.38
ꢂ0.38
—
ꢂ0.26
ꢂ0.29
—
ꢂ1.68
ꢂ1.70
ꢂ1.93
ꢂ1.90
ꢂ1.93
—
TPP
Zn-1
Zn-2
Zn-TPP
7
Acknowledgments
The authors thank Ms. Toshiko Muneishi at Osaka University for
the measurement of the NMR spectra. This work was partially sup-
ported by a Grant-in-Aid for Scientific Research on Priority Areas
—
a
E(DÅ+/D) ꢂ E(A/AÅꢂ) ꢂ E00, where E00 is the energy of photoexcitation.