Yasuhiro Morisaki, Yoshiki Chujo et al.
spectra of biphenyl and p-ter-
phenyl. Biphenyl exhibited
a broad absorption peak (Fig-
ure 4A), whereas 4 exhibited
a peak with a vibronic struc-
ture. In addition, the absorption
peak edge of
4 was batho-
chromically shifted compared
with that of biphenyl. As shown
in Figure 4B, the spectrum of 7
also exhibited a vibronic struc-
ture, which was bathochromi-
cally shifted in comparison with
that of p-terphenyl. These re-
sults are consistent with the
suppression of the rotary
motion of the phenylene rings
by the o-carborane skeleton. p-
Electrons are more effectively
delocalized through the highly
planar oligophenyl moieties
fixed by o-carborane than the
corresponding oligophenyls.
Photoluminescence
(PL)
Figure 3. The HOMO/LUMO orbitals and their energy levels calculated at the B3LYP/6-31GACHTNUTRGNE(NUG d,p) level of
theory for compound 4, 9,10-dihydrophenanthrene, biphenyl, and phenanthrene.
spectra of 7 and p-terphenyl are
shown in Figure S18 in the Sup-
porting Information (in CHCl3;
1.0ꢃ10À5 m). The PL spectrum
phenyl (5.37 eV) since the phenyl rings of biphenyl are
twisted due to the repulsion of hydrogen atoms. The highly
coplanar biphenyl moiety of 4 narrows the energy band gap
in comparison with 9,10-dihydrophenanthrene. The highest
occupied molecular orbital (HOMO) and lowest unoccupied
molecular orbital (LUMO) levels of 4 were estimated to be
À6.55 and À1.65 eV, respectively; these values were lower
than those of the other compounds examined. Since a contri-
bution of the electrical perturbation of the o-carborane skel-
eton to the biphenyl moiety was not observed, the deep
HOMO and LUMO levels arose from the electron-with-
drawing feature of o-carborane via the inductive effect. The
LUMO energy level of 4 was estimated from the cyclic vol-
tammogram (CV) peak onset potentials measured in the
DMF solution, as shown in Figure S15 in the Supporting In-
formation. A reduction signal with a peak onset at À1.2 V
(vs. ferrocene/ferrocenium) appeared, whereas no peak was
observed in biphenyl.[13]
of 7 exhibited a clear vibrational structure, and 7 emitted
bright purple fluorescence with a PL quantum efficiency
(FPL) of 0.52.[14] The Stokes shift was considerably small; the
absorption peak at 336 nm (Figure 4B) and the PL peak at
337 nm (Figure S18, Supporting Information) indicated a 0–
0 transition band. On the other hand, the PL peak top of p-
terphenyl appeared at 340 nm with a higher FPL of 0.93. A
broad vibrational PL spectrum of p-terphenyl was observed,
thus suggesting that similar structures of p-terphenyl moiet-
ies in both 7 and p-terphenyl are formed in the excited
state. To understand the decrease in FPL of 7 (=0.52), PL
measurements in a frozen medium were carried out (in 2-
MeTHF; 1.0ꢃ10À5 m at 77 K), as shown in Figure S19 in the
Supporting Information. The PL intensity of 7 increased ap-
parently at 77 K; therefore, the main non-radiative deactiva-
tion process is caused by the molecular motion of the o-car-
borane moiety rather than by an intramolecular CT process.
In conclusion, the synthesis, characterization, and proper-
ties of oligophenyl-fused o-carboranes have been described.
Owing to the effect of the o-carborane unit, high coplanarity
of the oligophenyl moieties was achieved. As a result, exten-
sion of p-conjugation, small Stokes shift, 0–0 transition
band, and clear vibronic structures in UV and PL spectra
were observed. In addition, o-carborane acted as a strong
electron-withdrawing group; in particular, o-carborane with-
drew electrons inductively. o-Carborane decreased both
HOMO and LUMO levels of oligophenyls without provid-
ing electronic perturbation. The energy levels of p-terphen-
yl-fused o-carboranes were lower than those of the corre-
In the case of the molecular orbitals of 7, a similar ten-
dency as for 4 was observed (see Figure S16 in the Support-
ing Information). The orbitals of 7 were identical to those of
5,6,12,13-dibenz
energy band gap (4.18 eV) was similar to that of 5,6,12,13-
dibenz
ACHTUNGTRENNUNG[a,h]anthracene and p-terphenyl, and the
[a,h]anthracene (4.26 eV). Deep HOMO (À6.53 eV)
and LUMO (À2.35 eV) energy levels were estimated, which
were derived from the inductive electron-withdrawal of o-
carborane.
UV/Vis absorption spectra of compounds 4 and 7 in
CHCl3 (1.0ꢃ10À5 m) are shown in Figure 4 together with the
Chem. Asian J. 2014, 9, 1247 – 1251
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