Angewandte
Chemie
[12]
[15]
Nuclear independent chemical shift (NICS) values at
the center of each of the ring segments A, B, C, and D were
calculated with the GIAO method at the B3LYP/6-311 +
G(d,p) level to be + 6.82, À7.52, À9.66, and À7.68 ppm,
respectively (Figure 2a). The calculated positive NICS(0)
value in ring A may be regarded as an indication of its
antiaromaticity being derived from COT, as discussed for
omatic porphyrinoids are not detected for 1. The Stokes
À1
shift is only 175 cm , thus indicating a rigid structure in the
excited state. In line with these absorption and emission
features, TD-DFT calculations have indicated intense degen-
erate bands with f = 0.22 at 399 nm to be ascribed to HOMO–
LUMO and HOMO-1–LUMO transitions. To gain further
insight into the frontier orbital diagrams, the magnetic
circular dichroism (MCD) spectrum of 1 was measured in
THF. The spectrum exhibits a positive-to-negative sign
sequence (negative Faraday A term) corresponding to the
main absorption at 416 nm, which indicates that the absorp-
tion bands consist of transitions from degenerate orbitals
(HOMO and HOMO-1) to a nondegenerate orbital (LUMO;
Figure 3b). Overall, these characteristics of 1 suggest an
aromatic-like character despite the presence of the central
planar COT. On the basis of frontier MO profiles it is
considered that the electronic properties of 1 stem from
peripheral aromatic segments (Figure S7-6).
[2–4]
other heterocirculenes.
However, the observed antiaro-
maticity in 1 is not as strong as the large positive NICS(0)
[6a]
value (+ 35.71 ppm) at the center of porphyrin sheet 3.
Examination of various substructures of 1 such as D -
4h
symmetric COT, tetrapyrrole 6, and [8]radialene 7 has
revealed that the positive NICS(0) value decreases with
elongation of the CÀC bond lengths around the COT
[
13]
structure. Therefore, the moderate positive NICS(0) value
and weakened antiaromaticity at ring A of 1 may be ascribed
[14]
to its “stretched” COT segment.
Figure 3a shows the UV/Vis absorption and emission
spectra of 1 and 5. Cyclic tetrapyrrole 5 exhibits a broad
absorption band at 326 nm and a broad fluorescence in the
To investigate the excited-state properties of 1 and 5, we
measured the dynamics of the S state by using the TCSPC
1
range 400–650 nm (F = 0.27) in THF. Interestingly, solid 5
(time-correlated single photon counting) technique (Fig-
ures S8-1 to S8-9). In the case of 5, we could observe
biexponential decay profiles and two time constants were
estimated to be around 1 and 5 ns. Moreover, the ratio
between the two components is slightly different depending
on the probe wavelength used. The fast decay component
corresponding to 1 ns is too slow to be assigned as structural
relaxation dynamics. As mentioned above, however, the
various conformers of 5 that exist at both room temperature
and even À808C probably give rise to the probe wavelength
dependent biexponential decay. To gain further insight into
this feature, we measured the fluorescence decay of 5 at 77 K
to reduce structural heterogeneity. As a result, we found that
the biexponential decay of 5 becomes a single exponential
decay with a lifetime of around 5.1 ns, regardless of the probe
wavelength.
F
emits fluorescence in the range 450–700 nm with F = 0.15
F
(
Figure S6-2). Compound 1 exhibits vibronic-structured
absorption bands at 390 and 413 nm and their mirror-image
sharp emission bands at 416 and 441 nm with a high quantum
yield (F = 0.55) in THF. Importantly, weak absorption tails
F
in the lower-energy region that are characteristic of antiar-
In the case of 1, the excited-state lifetime was estimated to
be 3.8 ns, with a single exponential decay. The measured
II
excited-state lifetime of 1 is much longer than that of the Zn
porphyrin sheet (1.1 ps) measured by the transient absorption
[6a]
II
technique. Considering that the Zn porphyrin sheet shows
antiaromaticity above the COT core and nonfluorescent
behavior, the well-resolved absorption/fluorescence spectra,
high fluorescence quantum yield, and long excited-state
lifetime of 1 strongly support its overall aromatic feature
being induced by the weakened antiaromatic character of the
central COT.
Finally, the fabrication of 1 was examined. Changes in the
absorption spectrum of 1 were observed upon addition of
tetrabutylammonium fluoride (TBAF), presumably because
of deprotonation of the NH protons (Figure S6-4). On the
basis of this observation, 1 was treated with an excess of
iodobutane in the presence of sodium hydride for 24 h at
room temperature to afford tetra-N-butylated tetraaza-
[
8]circulene 8 in 77% yield (Scheme 3). This product shows
improved solubility in common solvents, such as dichloro-
methane, chloroform, acetone, and benzene, which would
promise its further application as discotic liquid-crystalline
Figure 3. a) UV/Vis absorption (solid) and fluorescence (dashed) spec-
tra of 5 (gray) and 1 (black) in THF. b) MCD (top) and UV/Vis
[2c]
(bottom) spectra of 1 and 8 in THF.
mesogens, for example.
The structure of 8 has been
Angew. Chem. Int. Ed. 2015, 54, 10639 –10642
ꢀ 2015 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim