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R. Wang et al. / Tetrahedron Letters 54 (2013) 5307–5310
3 also showed favorable photochromism in hexane. Upon irradi-
ation with 297 nm light, the colorless solutions of 2o and 3o
turned orange and yellow. The absorption maxima were observed
at 494 and 455 nm, respectively (Fig. S1, SI). The colored solutions
of 2c and 3c could be decolorized upon irradiation with visible
light (k >500 nm). In the photostationary state (PSS), the photo-
conversion ratios from the open-ring to the closed-ring isomers
of 1–3 were evaluated by HPLC analysis (Fig. S2, SI), with the val-
ues of 32% for 1, 36% for 2, and 77% for 3. In PMMA films, 1–3
showed similar photochromism. But the absorption maxima of
the closed-ring isomers 1c–3c in PMMA films are much longer
than those in hexane. The red shift values are 13 nm for 1c,
12 nm for 2c, and 29 nm for 3c. The phenomena may be ascribed
to more planar structures and stabilization of molecular arrange-
ment of 1–3 in solid state.15
The photochromic features of 1–3 in both hexane and PMMA
films are summarized in Table 1. The results showed that the het-
eroaryl moiety significantly affected their photochromic proper-
ties, such as the absorption maxima, molar absorption
coefficients, and cyclization/cycloreversion quantum yields.
Among 1–3, the absorption maxima of the closed-ring isomers
remarkably increased in the order of benzofuryl < benzothie-
nyl < indolyl. Among the three analogs, the diarylethene with an
indole moiety (1) has the biggest visible absorption peak, molar
absorption coefficient, and cycloreversion quantum yield, but the
lowest cyclization quantum yield. Replacing the indole moiety
with a benzothiophene moiety (2), the absorption maximum and
the cycloreversion quantum yield decrease evidently, but the cycli-
zation quantum yield showed a minor increase. When the same
position has a benzofuran moiety (3), the molar absorption coeffi-
cient was still significantly lower than that of diarylethene 1. Its
absorption maximum and the cycloreversion quantum yield fur-
ther decreased whereas the cyclization quantum yield was notably
enhanced. Compared with the indole moiety (1), the absorption
maximum of 3 showed a notably hypsochromic shift with 80 nm.
The results indicated that the benzofuran ring could effectively
shift the absorption maximum to a short wavelength. In addition,
the molar absorption coefficients of both the open-ring and
closed-ring isomers varied with the same trend. They decreased
in the order of 1 > 3 > 2. Compared to those of 1, the cyclization
quantum yield of 3 was two fold larger but its cycloreversion quan-
tum yield was only one third of 1. As mentioned above, the photo-
chromic features of 1–3 were distinctly different. Compared with
the substituent effects, the heteroaryl group played a vital role dur-
ing the process of photoisomerization for the diarylethenes with a
similar photochromic skeleton. The possible reason may be that
the heteroaryl groups are directly connected to the central cyclo-
pentene ring, and can be available to participate in the photoin-
duced cyclization reaction. Additionally, in comparison with
symmetrical diarylethenes,4a,11f,12,16 the naphthalene-containing
diarylethenes with different heteroaryl moiety could significantly
decrease the absorption maximum of the closed-ring isomers and
the cycloreversion quantum yield. The results could be a useful
strategy for developing photochromic diarylethenes with shorter
absorption wavelength.
Scheme 1. Photochromism and color changes of diarylethenes 1–3 in hexane
(C = 5.0 ꢀ 10ꢁ5 mol Lꢁ1).
Br
NBS,THF
273 K
R
F
F
R
4a: R = N
4b: R = S
4c: R = O
F
F
F
F
5a: R = N
5b: R = S
5c: R = O
n-BuLi/THF
195 K
F
F
F
F
F
F
Br
R
1o: R = N
2o: R = S
3o: R = O
C5F8,195 K
n-BuLi/THF
F
6
7
Scheme 2. Synthetic route for diarylethenes 1o–3o.
coupled with the compound 78d to give diarylethenes 1o–3o,
respectively. Their structures were confirmed by elemental analy-
sis, NMR, and IR (Supplementary Information, SI).13
Diarylethenes 1–3 exhibited typical absorption changes upon
alternating irradiation with UV and visible light in both hexane
and polymer matrix at room temperature. As shown in Figure 1,
1o exhibited a sharp absorption peak at 281 nm (
e
, 1.22 ꢀ 104 -
L molꢁ1 cmꢁ1), which was arisen from p⁄ transition.14 Upon
p
?
irradiation with 297 nm UV light, the colorless solution of 1o
gradually turned purple (Scheme 1), and a new absorption max-
imum was observed at 535 nm (
e
, 1.09 ꢀ 104 L molꢁ1 cmꢁ1) due
to the formation of the closed-ring isomer 1c. Upon exposure to
visible light (k >500 nm), the purple color was bleached entirely,
indicating that 1c returned to the initial state 1o. Similarly, 2 and
0.6
3o
2o
0.4
The thermal stability of diarylethenes with two naphthalene
moieties is very excellent, and the absorptance of the closed-ring
isomers remains almost constant for more than 500 h even at
343 K.16 Therefore, it can be expected that the unsymmetrical
diarylethenes with a naphthalene moiety also exhibit good ther-
mal stability. The thermal stability of the open-ring and closed-ring
isomers of 1–3 was examined at both room temperature and
351 K. Storing these solutions in the dark and then exposing them
to air for more than a week at room temperature, no changes in
color and absorption spectra of 1–3 were observed. When these
ethanol solutions were heated under reflux (351 K) for 8 h in
PSS 3
1o
PSS 1
PSS 2
0.2
0.0
300
400
500
600
Wavelength (nm)
Figure 1. Absorption spectral changes of diarylethenes 1–3 by photoirradiation in
hexane (C = 5.0 ꢀ 10ꢁ5 mol Lꢁ1) at room temperature.