D. Kim, T. K. Chandrashekar et al.
CDCl3 leads to small downfield shift in the pyrrole and thio-
phene b-CH protons in the H NMR spectrum of 3. On the
we could assume that the hybrid character of bridged hexa-
phyrin cause two transitions; one is porphyrin-like transi-
tion, while the other is a hexaphyrin-like transition. Based
on a comparison of the absorption spectra with the calculat-
ed results, we could assume that the peak at 433 nm is origi-
nated from porphyrin, that around at 531 nm region is
mixed with hexaphyrin and porphyin, and one at 917 nm is
caused by hexaphyrin. This hybrid character of 3 is also sup-
ported by the AICD plots, which show the 3D image of de-
localized electron densities with a scalar field and illustrates
the paramagnetic term of the induced current density; aro-
matic molecules show clockwise current density and antiaro-
matic species show counter-clockwise current density. The
AICD plot shows that the ring currents flow along not only
the hexaphyrin frame but also the bridged thiophene (Sup-
porting Information). From this result, we could assume that
the overall ring current density consist of the ring current
flows, which are mainly localized on hexaphyrin and partial-
ly localized on porphyrin. On the other hand, the MO pic-
ture for 4 (Supporting Information) indicates that the elec-
tron density distribution is mainly localized on the 26p hexa-
phyrin skeleton and an intense Soret-like band observed at
567 nm is consistent with this conclusion.
For the evaluation of aromaticity, we calculated the
NICS(0) values both within the inner porphyrin cavities and
outside (Supporting Information). To avoid the local aro-
matic effect from the bridging thiophene ring, we chose to
calculate the NICS values at the centers of two porphyrin-
like cavities rather than at the center of the hexaphyrin skel-
eton. The highly negative NICS(0) values observed (for 3,
À14.0 and À13.3 ppm; for 4, À18.3 and À17.9 ppm) at the
inner cavities and positive values outside strongly suggest
the aromatic nature of the bridging hexaphyrins. The rever-
sible/quasi reversible redox waves from the cyclic voltam-
metric experiments further confirm such a conclusion.
The final confirmation of structures of 3 and 4 came from
the single-crystal X-ray structural analyses (Supporting In-
formation). In both 3 and 4, the molecule is located on a
crystallographic two-fold axis. As predicted from the spec-
tral analyses, 3 contains two thiatripyrrin units, while 4 con-
sists of two selenatripyrrin units and both the units are indi-
vidually bridged by a thiophene moiety and the remaining
four meso positions are occupied by the mesityl groups (Fig-
ure 4a). The bridged thiophene in 3 and 4 is in positional
disorder, where two of the thiophene units overlap each
other. Analysis of crystal structure reveals that the thiatri-
pyrrin units in 3 (N1-S1-N2) are slightly deviated from the
mean plane with deviations of 10.28, 3.38 and 5.78, where the
selenatripyrrin in 4 (N1-Se1-N2) units are hardly deviated
from the plane. However, the bridged thiophene unit in 3
and 4 are deviated by 498 and 738, respectively (Figure 4b),
while the meso-mesityl rings in 3 and 4 are almost perpen-
dicular (89.38; 81.58 for 3 and 83.48; 78.18 for 4) to the mean
macrocyclic plane. Further, one of the meso-mesityl CH
groups is in intermolecular hydrogen bonding interaction
with meso-mesityl p-cloud (C23-H23c···Mes(p)) of the adja-
cent molecule that was used to generate the one-dimension-
1
contrary, the b-CH protons of bridging thiophene experi-
ence shielding of 1.2 ppm upon addition of 2 equiv of TFA.
However, excess addition of TFA (4 equiv) leads to down-
field of the b-CH protons, and they appear at 4.2 ppm (Sup-
porting Information, Figure S14). These observations clearly
suggest that the conformation of the bridging thiophene
group is sensitive to protonation, and significant changes
occur in the conformation upon protonation.
The protonated inner NH peaks were observed only at
low temperature (183 K) (Supporting Information). On
adding 2 equiv of TFA, five different NH peaks were ob-
served in the range of À1 to À7 ppm, suggesting the pres-
ence of different species that are chemically and magnetical-
ly inequivalent. On adding 4 equiv of TFA, a single peak at
À4.7 ppm was observed, which indicates the saturation of
protonation centers. Furthermore, the increase in the
number of meso-mesityl methyl and pyrrole peaks (Support-
ing Information) is attributed to 1) a lack of rotational free-
dom owing to the internal bridging thiophene; and 2) a low-
ering of the symmetry, making the meso-mesityl rings ineq-
uivalent. The 1H NMR spectrum of 4 at 298 K shows the
similar pattern as 3. The b-CH protons of the bridging thio-
phene in 4 are more shielded relative to 3 and resonate at
1.35 ppm.
In an effort to understand the characteristics in the ab-
sorption spectra, we calculated molecular orbitals (MO)
based on X-ray crystal structures and transition energies by
TD-DFT method using Beckeꢁs three-parameter hybrid ex-
change functional and the Lee–Yang–Parr correlation func-
tional (B3LYP) employing the 6–31G basis set for 3
(Figure 3). According to the frontier orbital diagram, the
MOs of bridged hexaphyrin consists of the summation of
the MOs in which electron density distribution is localized
on porphyrin (HOMOÀ1, HOMOÀ2) and the MOs in
which electron density distribution is localized on hexaphyr-
ins (LUMO). The MOs where electron density distribution
of 3 is localized on porphyrin give rise to porphyrin-like
transition at 433 nm. Furthermore, the MOs where electron
density distribution is localized on porphyrin moiety also
affect hexaphyrin-like transition at 917 nm. From these data,
Figure 3. Energy level diagram and molecular orbitals of 3.
1888
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Chem. Eur. J. 2013, 19, 1886 – 1890