4076
Y. Lu, J. S. Moore / Tetrahedron Letters 50 (2009) 4071–4077
0.8
0.6
0.4
0.2
0.0
1.2
1.0
10
11
12
10
11
12
0.8
0.6
0.4
0.2
0.0
200
300
400
500
600
700
800
Wavelength (nm)
200
250
300
350
400
450
500
550
Wavelength (nm)
Figure 8. Normalized fluorescence spectra of 10–12 in dichloromethane (5.1 lM,
25 °C). The excitation wavelengths were set to the kmax (abs) of each compound (10,
282 nm; 11, 341 nm; 12, 377 nm).
Figure 7. UV–vis absorption spectra of 10–12 in dichloromethane at 25 °C. The
spectra are normalized to 5.1 lM concentration.
two bands provide the characteristic vibronic spectral pattern
responsible for the chromophore nature and planarity of 11,
respectively.19,20 The absorption maxima around 272 nm is due
to the oligophenylene chromophore, and the absorption in the
other UV region around 342 nm is due to the planarization of the
oligophenylene core to generate the semi-fused ring with added
conjugation. Similarly, in the case of 12, the absorption in the UV
region (230–325 nm) represents the oligophenylene chromophore.
Table 2
Absorption maxima and extinction coefficients of 10–12
Compd
kmax (abs), nm
e
, MÀ1 cmÀ1
10
229.0
282.0
6.90 Â 104
1.41 Â 105
11
12
205.5
234.0
271.5
341.5
389.5
402.5
6.47 Â 104
8.61 Â 104
1.23 Â 105
1.47 Â 105
4.12 Â 104
4.12 Â 104
The next absorption maxima of 12 (377 nm, 1.24 Â 105 MÀ1 cmÀ1
)
is bathochromically shifted compared to that of 11 (342 nm,
1.47 Â 105 MÀ1 cmÀ1) with a slight decrease in the absorption
intensity upon extension of the conjugation. For comparison, the
absorption spectrum of the reference compound 10 is also shown
in Figure 7, which contains only one distinct UV band (240–
350 nm) corresponding to its nonplanar polyphenylene chromo-
phore as that in 11 and 12.
225.5
262.5
377.0
419.5
8.04 Â 104
1.39 Â 105
1.24 Â 105
3.31 Â 104
The fluorescence spectra of 11 and 12 generally lacked fine fea-
tures possibly due to the high concentration used for the excitation
experiments.21 As shown in Figure 8, the emission maxima of 11
and 12 exhibited bathochromic shifts compared to that of precur-
sor 10 in dichloromethane (10: kem = 370 nm, colorless; 11:
pendent of 12. 1H NMR was used to monitor the product distribu-
tion of three individual reactions under the medium concentration
condition with varied reaction times: 70 min, 80 min, and 90 min
(Fig. 6). The reaction time within this 20 min window had a dra-
matic effect on the product distribution. The majority of 11, which
appeared to be the main product in the 1H NMR spectrum at
70 min, converted to fully cyclized 12 at 90 min. However, cyclode-
hydrogenation reaction pathways are known to be complex:13 the
sensitivity of the reaction time, oxidant loading, and addition rate,
as well as reaction concentration all lead to the difficulty in achiev-
ing accurate control of the product distribution. However, the com-
parison data demonstrate that 11 is a kinetically favored reaction
intermediate instead of a thermodynamically stable product. To
support this statement further, purified compound 11 was sub-
jected to Scholl condensation reaction to confirm that 11 can be
converted to completely cyclized 12. 1H NMR and ESI-MS results
revealed that by using 22.6 equiv of FeCl3, the majority of 11 was
transformed into 12 after 40 min. Thus, we conclude that 11 is in-
deed a Scholl reaction intermediate. Although the generation of
semi-fused HBC structure had been recently reported in the form
of a nitrogen-containing HBC, such analog was shown to be a ther-
modynamically stable product that cannot undergo further trans-
formation into the fully cyclized structure.13
kem = 441 nm, UF = 0.28, yellow-green; 12: kem = 520 nm, UF
=
0.08, yellow). The fluorescence quantum yield of 11 is markedly
higher than that of 12. Interestingly, the solubility of 11 was found
to be lower than that of 12. The finding of the non-heteropolyaro-
matic, semi-fused 11 not only supports the stepwise Scholl con-
densation pathway leading to HBCs demonstrated earlier by
Müllen and co-workers,5 but also offers a new generation of
conjugated fluorescent molecules. We imagine that introduction
of such unique structures into polymer films would create new
opportunities for developing optical and electronic materials from
semi-fused HBCs.
Acknowledgments
This work was supported by the National Science Foundation
Science (CHE-0642413) and the NSF Science Technology Center
of Advanced Materials for the Purification of Water with Systems
(WaterCAMPWS) (Grant No. CTS-0120978). We thank Furong Sun
from the Mass Spectrometry Laboratory, SCS, University of Illinois
for valuable expertise in ESI and MALDI-MS characterization
experiments. Y.L. thanks Dr. Mitch Schultz for helpful discussions.
The semi-fused 11 provides an opportunity to compare it with
12 for investigating the potential interesting photophysical proper-
ties and applications of semi-HBC structures. The UV–vis spectra of
10–12 in CH2Cl2 are presented in Figure 7, and the absorption max-
Supplementary data
ima (kmax) and molar extinction coefficient (e) are collected in Ta-
ble 2. Based on the spectra, the absorption of nonplanar 11 has two
distinct bands in the UV region (245–305 nm, 305–370 nm). These
Supplementary data associated with this article can be found, in