D. Kim, A. Osuka et al.
In the cyclic voltammogram of 5, the irreversible wave at
0.32 V corresponds to the oxidation of the 4-dimethylamino-
phenyl moiety, as referring to the relevant data.[14] Thus, the
electrochemical HOMO–LUMO gap of 5 is 2.36 eV. Similar-
ly, the first oxidation potential of 7 was observed at À0.17 V,
which is ascribed to the oxidation of the ferrocene moiety.
The electrochemical HOMO–LUMO gap of 7 is much
smaller, being 1.84 eV.
tial function with a time constant of 1.54 ns and a very short
time constant (t <30 ps), suggesting the presence of an ad-
ditional decay channel from their S1-excited states. The ab-
sence of a measureable fluorescence of 7 provides further
support for existence of efficient nonradiative decay chan-
nel. While preliminary experiments indicated a non-fluores-
cent nature of subporphyrin 13, its facile hydrolytic reactivi-
ty hampered detailed studies of its fluorescence, since hy-
Table 2 summarizes the optical properties of subporphyr-
ins 1–13. Subporphyrins 2–11 show Soret-like bands in the
range of 382–385 nm and Q-like bands in the range of 501–
508 nm. Soret-like bands of 12 and 13 are observed at 379
and 389 nm, which are slightly blue- and red-shifted, respec-
tively, as compared with those of 2–11. These data suggests
that the effects of the axial carbon ligands on the absorption
spectra of the subporphyrins is negligible, as seen for the
drolysis produced fluorescent BACTHNGUTERNNU(G hydroxo)subporphyrin. The
efficient fluorescence quenching observed for 5 and 7 may
be attributed to intramolecular electron transfer from the
axial group to the subporphyrin S1-state. Relevant driving
force values of the electron transfer have been estimated to
be À0.51 and À0.99 eV for 5 and 7, respectively.[15] These
large negative driving forces support the fact that the intra-
molecular electron transfer processes are responsible for the
fluorescence quenching.[16]
To understand the electrochemical and optical properties,
MO calculations were performed at the B3LYP/6-
311G(d) level using the Gaussian 09 package[17] (see Fig-
ure S7 in the Supporting Information). Subporphyrin 1 has
a2u-like HOMO, a1u-like HOMOÀ1, and a couple of degen-
erate eg-like LUMO and LUMO+1 levels. Subporphyrins
2–13 show essentially the same orbital features, except the
cases of 5, 7, and 10, in which HOMOs are localized at the
axial groups, reflecting their electron-donating properties.
These data are consistent with the electrochemical measure-
ments, and support the fact that the fluorescence quenching
is ascribed to the intramolecular electron transfer from the
axial group to the S1-state of the subporphyrins.
Finally, it is worth noting that the optical properties of 5
contrast with those of meso-(4-dibenzylaminophenyl) sub-
porphyrin 14[5a] and meso-(4-dimethylaminophenyl)ethynyl
subporphyrin 15,[18] both of which exhibit split Soret-like
bands and red-shifted and enhanced fluorescence. In subpor-
phyrins 14 and 15, conjugative interactions of the electron-
donating meso-substituents are responsible for the perturbed
absorption spectra and fluorescence spectra. In other words,
the electronic interactions of 4-dibenzylaminophenyl and (4-
dimethylaminophenyl)ethynyl substituents with the subpor-
phyrin core are strong enough to create an expanded chro-
mophoric conjugation by including meso-substituents. In
contrast, the axial 4-dimethylaminophenyl group in 5 is en-
tirely non-conjugated with the subporphyrin core due to the
nodal character of the central B atom and the orthogonal
orientation. This situation is favorable for state-to-state dy-
namics such as intramolecular electron transfer.
[10e]
À
subphthalocyanine bearing a B C bond.
hand, the fluorescence quantum yields of subporphyrins
On the other
À
bearing a B C bond are variable. While many of the B-fab-
ricated subporphyrins exhibit fluorescence quantum yields
(FF) in the range of 0.10–0.16, which are comparable to that
of 1, subporphyrins 5 and 7 bearing a strongly electron-do-
nating axial group exhibit very small FF values and subpor-
phyrin 10 shows a slightly small FF value. The fluorescence
decays measured by time-correlated single photon counting
techniques in toluene obey a single exponential function in
most cases with the following time constants; 2.44 ns for 2,
2.31 ns for 3, 2.45 ns for 4, 1.99 ns for 6, 1.74 ns for 8, 2.45 ns
for 9, 1.53 ns for 10, 2.51 ns for 11, and 2.01 ns for 12, re-
spectively (see Figure S8 in the Supporting Information).
The fluorescence decay of 5 was analysed by a bi-exponen-
Table 2. Optical properties of subporphyrins 1–13.[a]
[b]
Cmpd
labs [nm] (e [105 mÀ1 cmÀ1])
372 460
(1.66) (0.12)
385 478
(1.36) (0.09)
384 478
(1.40) (0.09)
385 480
(1.31) (0.09)
385 481
(1.43) (0.09)
382 474
(1.36) (0.09)
383
(1.22)
383
(1.37)
385
(1.35)
385
(1.12)
382
(1.44)
379
(1.56)
389
(1.40)
[a] Measured in CH2Cl2. [b] Absolute fluorescence quantum yield
lem [nm]
FF
1
485
(0.09)
507
(0.13)
506
(0.13)
507
(0.13)
508
(0.14)
502
(0.12)
505
(0.09)
501
(0.12)
507
(0.13)
501
(0.10)
502
(0.12)
497
(0.12)
514
(0.10)
517
0.13
G
G
ACHTUNGTRENNUNG
2
541
544
546
546
538
542
534
545
541
546
528
–
0.16
R
ACHTUNGTRENNUNG
3
0.15
E
ACHTUNGTRENNUNG
4
0.14
N
ACHTUNGTRENNUNG
5
<0.01
0.12
N
ACHTUNGTRENNUNG
6
R
ACHTUNGTRENNUNG
7
<0.01
0.10
N
ACHTUNGTRENNUNG
8
N
ACHTUNGTRENNUNG
In summary, a convenient methodology for efficient axial
fabrication of subporphyrins has been developed by reaction
of B-(methoxo)triphenylsubporphyrin with Grignard re-
9
0.14
R
ACHTUNGTRENNUNG
10
11
12
13
0.087
0.15
E
ACHTUNGTRENNUNG
G
ACHTUNGTRENNUNG
0.12
N
ACHTUNGTRENNUNG
<0.01
G
ACHTUNGTRENNUNG
11160
ꢀ 2013 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2013, 19, 11158 – 11161