Angewandte
Communications
Chemie
cycle 2e and HCl. The DFT calculation shows that the
HOMO of B is mainly localized in the central stilbene moiety,
thus indicating the electron-donating nature of the phenyl
rings, which are favorable for reacting with the cation
reduced structural rigidity of the former. DSFIIFs exhibit the
absolute fluorescence quantum yields of 0.45 for 2b, 0.56 for
2e, and 0.45 for 2h, and are lower than the reported results of
[1,2-b]DSFIFs (Scheme 1a, 0.62–0.70). It is worth noting that
the DSFIIF 2I, having two electron-withdrawing ester groups
at the central indeno[2,1-a]indene moiety, exhibits a red-
shifted absorption and emission maxima compared to other
DSFIIF derivatives. Interestingly, 2i is highly fluorescent with
electrophiles (see Figure S1). Either the FeO(OH) or Fe O3
2
additive may react with HCl to supply the fresh FeCl oxidant,
3
thus suppressing the partial decomposition of 1e by HCl, and
it is crucial for achieving high yields of the dispirocycles.
The optical and electrochemical properties of the selected
dispirocycles 2 are summarized in Table 3 and Figure 2 (see
also Figures S2 and S3). The UV-vis absorption spectra of the
the absolute quantum yield of 0.94 in CHCl , thus implying
3
the distinct substituent effect of the ester group on the p-
conjugated indeno[2,1-a]indene moiety. The HOMO energy
levels of DSFIIFs were calculated from the oxidation
potentials by cyclic voltammetry (CV) in CH Cl , and the
2
2
lowest unoccupied molecular orbital (LUMO) energy levels
were estimated from the optical bandgap and HOMOs. The
HOMO energy levels of 2b, having two electron-donating
tert-butyl groups at the indeno[2,1-a]indene moiety is
À5.49 eV, similar to the reported [2,1-a]DSFIF(tBu)
[
24]
(
À5.48 eV, Scheme 1a). The nonsubstituted 2e (À5.68 eV)
and 2h (5.62 eV), having four tert-butyl substituents at the
fluorene moieties, exhibited slightly lower HOMOs than that
of 2b, and are similar to the reported values (À5.76 eV,
À5.66 eV, 5.61 eV) of the three [1,2-b]DSFIF isomers (Sche-
[15,24]
me 1a).
The LUMO energy levels of 2b, 2e, and 2h,
estimated to be in the range of À2.10 to À2.23 eV, are very
near to the reported DSFIF series. 2i shows both low HOMO
and LUMO energy levels of À5.95 eV and À2.80 eV with
a narrow energy bandgap of 3.15 eV resulting from the two
electron-withdrawing ester groups at the indeno[2,1-a]indene
moiety.
Figure 2. UV-vis spectra (left; solid line) and fluorescence spectra
(right; solid line) of 2b, 2e, 2h, and 2i in chloroform solution.
Normalized UV-vis absorption of spin-coated thin films on the quartz
In conclusion, we have developed a novel and highly
plates (dashed line) at room temperature. F =quantum yield.
f
efficient FeCl -mediated oxidative spirocyclization of 1,2-
3
di(9H-fluoren-9-ylidene)-1,2-diphenylethanes under mild
reaction conditions. A new class of di-spirolinked indeno-
[2,1-a]indene p-conjugated systems having a wide range of
functional groups have been synthesized in very high yields
with the highest fluorescence quantum yield of 0.94 for the
ester-substituted dispirocycle. The results led to the conclu-
sion that the present mechanism involved two one-electron
oxidations and a dication-induced Friedel–Crafts spirocycli-
zation pathway. This protocol also can be applicable for the
construction of non-spirolinked dihydroindenoindenes. The
present method provides not only a novel and valuable
spirocycle synthetic tool, but also a new type of spirolinked p-
conjugated system which is expected to be highly applicable
in the field of optoelectronics.
nonsubstituted (2e) and tBu-substituted (2b and 2h) DSFIIFs
exhibit bands of the central indeno[2,1-a]indene moiety in the
range of l = 300–360 nm in chloroform, and they are very
similar to the [1,2-b]DSFIFs having similar substituents at the
central dihydroindeno[1,2-b]fluorene moiety as reported by
[15,24]
Poriel, Rault-Berthelot et al. (Scheme 1a).
Thin-film
absorption maxima of 2b, 2e, and 2h, recorded on spin-
coated films on the quartz plates, are slightly red-shifted
compared to the corresponding solution absorption maxima,
thus implying very weak intermolecular interactions in solid
state. The photoluminescence spectra of the present DSFIIFs
show Stock shifts of 15–17 nm, which are larger than that of
[15,24]
[
1,2-b]DSFIF analogues (2–3 nm),
thus indicating the
Table 3: Selected optical and electrochemical properties of DSFIIFs
[
a]
[b]
[c]
[d]
ox
[e]
opt
[f]
[g]
[h]
DSFIIF
labs [nm]
labs [nm]
lem (lexc) [nm]
Ff
E
[V]
DE [eV]
HOMO [eV]
LUMO [eV]
2
2
2
2
b
e
h
i
358, 341, 326, 263
352, 336, 315, 261
353, 336, 318, 305, 268, 254
386, 366, 350, 325, 310, 299
359
356
353
390
390 (340)
382 (320)
382 (340)
420 (340)
0.45
0.56
0.45
0.94
0.91
1.11
1.04
1.29
À3.39
À3.45
À3.44
À3.15
À5.49
À5.68
À5.62
À5.95
À2.10
À2.23
À2.18
À2.80
[
[
a] UV-vis absorptions were measured in chloroform. [b] UV-vis absorptions were measured using as-spun thin films on the quartz plates.
c] Fluorescence maxima were measured in chloroform. [d] Absolute fluorescence quantum yield (F ) was measured by a photon-counting method
f
opt
using an integration sphere. [e] Oxidation potential (vs Ag/AgCl) was measured by cyclic voltammetry in CH Cl . [f] Optical bandgap (DE ) was
2
2
estimated from the contact between the UV-vis absorption and the fluorescence spectra. [g] HOMO was calculated from the oxidation potential.
h] LUMO was calculated from the HOMO energy and the optical bandgap.
[
262
ꢀ 2016 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2016, 55, 259 –263