S. Yamaguchi et al.
COMMUNICATION
tion at 900 nm.[19] These
d
values are approximately twice
as high as that of the reference
compound 9 (d=216 GM at
900 nm). These results demon-
strate that the zwitterionic
modulation of the distyrylben-
zene chromophore is useful for
the design of high-performance
TPA materials, while the bridg-
ing pattern does not signifi-
cantly affect the TPA proper-
ties, and dipolar 3 shows a
slightly larger d value among
the three DSB derivatives. Be-
sides, we found that the incre-
ment of the electron-donating
ability of the terminal borate
moieties in the BÀP+P+BÀ-
DSB 2 by replacing the ben-
zene rings with thiophene rings
resulted in a much larger TPA
cross section. The d value of
Figure 2. Energy diagrams and pictorial representations of the frontier MOs for the phosphonium- and borate-
bridged DSBs 1’–3’ and BTB 4’ calculated at the B3LYP/6-31G(d) level, and their lowest-energy transitions es-
timated by TD-DFT calculations at the B3PW91/6-31+G(d)//B3LYP/6-31G(d) level. Methyl and phenyl
groups were used instead of the cyclohexyl and mesityl groups in the corresponding compounds 1–4, respec-
tively. The trimethylsilyl groups were used instead of the triisopropylsilyl groups in 4.
tron-accepting phosphonium located at the inner positions
cancel the electronic effects of each other. Indeed, the
HOMO and LUMO of 3’ are mostly localized on the termi-
nal benzoborole and the terminal benzophosphole moieties,
respectively. These rather localized frontier MOs may en-
hance the intramolecular CT character and thus result in the
large Stokes shift.
the BÀP+P+BÀ-BTB 4 was 784 GM even upon excitation at
1200 nm. It is worth noting that there are only a few exam-
ples of excellent TPA materials that can be excited with a
NIR light, such as the highly polarized D-p-A type p-conju-
gated compounds[2b] and the oligomeric porphyrin deriva-
tives with inherently long-wavelength absorption bands.[4]
These facts clearly demonstrate that the present zwitterionic
modulation is also useful for attaining a large d value in the
NIR region.
In summary, we investigated the linear absorption, fluo-
rescence, and two-photon absorption properties of a series
of phosphonium- and borate-bridged distyrylbenzenes 1–3.
All these compounds showed larger d values compared to
the previously known TPA-active distyrylbenzene derivative,
regardless of the bridging patterns. Moreover, a large TPA
cross section, even upon excitation at 1200 nm, was also at-
tained in the thienyl-terminated derivative 4. These results
clearly demonstrate that the introduction of zwitterionic
bridges into the ladder p-conjugated framework is a power-
ful strategy for the molecular design of excellent TPA mate-
rials.
The replacement of the terminal benzene rings in the
BÀP+P+BÀ-DSB 2 with thiophene rings significantly affects
the linear absorption and fluorescence properties. The BÀP+
P+BÀ-BTB 4 has an absorption maximum at 620 nm in ben-
zene, which is nearly 90 nm longer than that of the DSB an-
alogue 2. Moreover, 4 exhibits an emission in the red to
NIR region with a lem value of 734 nm, although the fluores-
cence quantum yield is low (FF =0.021). As shown in
Figure 2, the DFT calculations of their model compounds 2’
and 4’ at the B3LYP/6-31G(d) level revealed that the
HOMO level of 4’ (À4.81 eV) is higher than that of 2’
(À5.21 eV), while their LUMO levels are comparable to
each other (À2.82 eV for 2’, and À2.81 eV for 4’). This fact
clearly demonstrates that the enhancement of the electron-
donating character of the terminal borate moieties by re-
placing the benzene rings with thiophene rings is responsible
for the significantly red-shifted absorption and fluorescence
bands.
Two-photon absorption properties for a series of zwitter-
ionic ladder bis(arylethenyl)benzenes 1–4 were evaluated by
the Z-scan method using a femtosecond optical parametric
amplifier.[16] The TPA cross sections d are also collected in
Table 1, together with the data of a representative quadru-
polar distyrylbenzene derivative 9[17] for comparison.[18] The
obtained d values of quadrupolar P+BÀBÀP+-DSB 1 and
BÀP+P+BÀ-DSB 2, and dipolar P+BÀP+BÀ-DSB 3 in ben-
zene, were 349, 469, and 476 GM, respectively, upon excita-
Acknowledgements
This work was partially supported by Grants-in-Aid (Nos. 17069011,
19675001, and 20750029) from the Ministry of Education, Culture,
Sports, Science, and Technology of Japan. H.Y. thanks the Research Fel-
lowships of the Japan Society for the Promotion of Science (JSPS) for
Young Scientists.
Keywords: boron · phosphorus · pi interactions · two-
photon absorption · zwitterions
468
ꢀ 2010 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Asian J. 2010, 5, 466 – 469