Communications
as Faraday B terms, which are indicative of the absence of a
To further support the absorption spectra and MO
calculations, electrochemical measurements were performed
on these compounds. A quasireversible one-electron oxida-
tion process and a reversible one-electron reduction process
are observed at 0.53 and À1.54 V (vs. Fc+/Fc), respectively, for
1 (see the Supporting Information). The first reduction
potential of 2 at À1.61 V is comparable with that of 1,
whereas the first oxidation potential at 0.15 V is shifted
negatively, and is indicative of a high-lying HOMO as
predicted by DFT calculations. This results in a decrease of
the potential energy difference (1.76 V for 2 and 2.06 V for 1),
which is in agreement with the large red shift of the Q band.
In summary, a novel subphthalocyanine analogue com-
prising an azaphenalene moiety was prepared according to
the same synthetic protocol employed for the synthesis of
APPcs.[12] This new species retained a 14p-electron aromatic
conjugation system despite the presence of a six-membered
ring unit in its conjugated system, and the electronic structure
was significantly altered as a result of the incorporation of the
azaphenanlene moiety. SubAPPc can absorb a wide range of
light energy, which is a useful property for functional dyes
employed in various fields. The introduction of azaphenalene
units is a promising method for modifying electronic struc-
tures and properties of Pc, SubPc, and their related com-
pounds. Further investigation using this approach is currently
underway.
threefold or higher symmetry axis, and these kinds of SubPc
molecules generally possess nondegenerated excited states.[19]
Although the molar absorption coefficient of 2 is about half of
that of 1, it should be emphasized that the absorption
spectrum of 2 covers a wide range in which neither general
Pc nor SubPc have absorption. This observation is particularly
favorable for photoenergy conversion processes because dyes
which effectively absorb a wide range of light energy are
strongly desired. Compound 2 also shows fluorescence at
718 nm with a Stokes shift of 197 cmÀ1, and the fluorescence
quantum yield (FF) of 0.18[20] and fluorescence lifetime (tF) of
3.6 ns are comparable with those of the general SubPcs.[2]
Molecular orbital calculations were performed using DFT
methods at the B3LYP/6-31G(d) level on model compounds
of 1 and 2 in which the peripheral substituents and axial ligand
were replaced with hydrogen atoms and a hydroxy group for
simplicity (Figure 3). The frontier orbitals of 2 show similar
Experimental Section
Preparation of 1 and 2: A suspension of 1,8-naphthalenedicarbonitrile
(90 mg, 0.5 mmol) and 4,5-di-p-tert-butylphenyloxyphthalonitrile
(1 equiv, 212 mg, 0.5 mmol) in 1-chloronaphthalene (2 mL) was
heated at 1908C for approximately 10 seconds. Then, a solution of
boron trichloride in n-heptane (1.0m, 1 mL, 1 mmol) was added by a
syringe under a nitrogen atmosphere and the mixture was heated at
1908C for another 5 min to give a blue/purple solution. Preparative
thin-layer chromatography (silica gel, F254, 60, eluent: CHCl3) was
employed to remove impurity and the purple and the blue fractions
were collected. These fractions were further purified by GPC-HPLC.
The first fraction (purple) to elute from the GPC was characterized as
a mixture of axially chloro- or hydroxy-substituted subphthalocya-
nines, and the second fraction (blue) was identified as a similar
mixture of subazaphenalenephthalocyanines. Finally the first and the
second fractions were treated with phenol at 1208C for 2 h in the dark,
respectively, and the products were further purified by column
chromatography on silica gel to provide axially phenoxy-substituted
subphthalocyanine (1) and axially phenoxy-substituted subazaphe-
nalenephthalocyanine (2) in 5.6% and 1.6% yields, respectively.
Characterization of subphthalocyanine (SubPc; 1): ESI-FT-ICR-
MS: m/z calcd for C90H89BN6NaO7 [M++Na]: 1399.6783; found:
1399.6778; 1H NMR (CDCl3, 400 mhz, 298 K): d = 8.25 (s, 6H; a-
benzo), 7.42 (d, 12H, J = 8.83 Hz; phenyl), 7.08 (d, 12H, J = 8.81 Hz;
phenyl), 6.74 (dd, 2H, J1 = 7.36 Hz, J2 = 8.35 Hz; axial meta-phenyl),
6.60 (t, 1H, J = 7.34 Hz; axial para-phenyl), 5.31 (d, 2H, J = 8.66 Hz;
axial ortho-phenyl), 1.37 ppm (s, 54H; tert-butyl); UV/Vis (CHCl3):
lmax (nm); e = 357 (16900), 528 (sh, 15600), 553 (sh, 28500), 573
(51400).
Figure 3. Frontier molecular orbital diagrams of 1 (left) and 2 (right).
density distribution patterns to those of 1, and coefficients are
found at the naphthalene moiety in the case of highest
occupied molecular orbital (HOMO) and LUMO + 1
(LUMO = lowest occupied molecular orbital). This results
in significant destabilization of the HOMO and an energy
difference between the LUMO and LUMO + 1 by 0.08 eV.
Furthermore, TDDFT calculations reveal two bands in the Q-
band region which mainly consist of transitions from the
HOMO to LUMO and LUMO + 1. The smaller HOMO–
LUMO energy gap of 2, therefore, explains the red shift of the
lower-energy Q band, and the substantial energy difference
between the LUMO and LUMO + 1 explains the splitting of
the Q bands. These calculation results are in good agreement
with the observed Faraday B terms in the MCD spectrum of 2.
Characterization of subazaphenalenephthalocyanine (SubAPPc;
2): ESI-FT-ICR-MS: m/z calcd for C74H66BClN6O5Na [M++Na]:
1187.4774; found: 1187.4768; 1H NMR (CDCl3, 600 mhz, 298 K): d =
8.77 (d, 1H, J = 7.37 Hz; naphthalene), 8.63 (d, 1H, J = 8.04 Hz;
naphthalene), 8.09 (m, 3H; naphthalene (1H) and a-benzo (2H)),
8.01 (s, 2H; a-benzo), 7.59 (m, 2H; naphthalene), 7.41 (m, 8H;
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2010, 49, 8000 –8003