28
J. YUAN AND Y. BAO
Table 1. Photochromic parameters of dithienylethene 1-3 in DCM at 298 K (2.0 ꢁ 10ꢂ5 mol/L).
kmax/nma
(e ꢁ 104)
Open
kmax/nmb
(e ꢁ 104)
PSSd
Uc
Compounds
uo-c
uc-o
1
2
3
246 (8.38)
247 (6.58)
357 (6.40)
518 (1.59)
544 (1.47)
596 (2.85)
0.356
0.232
0.526
0.0079
0.0065
0.0092
aAbsorption maxima of open-ring isomers;.
bAbsorption maxima of closed-ring isomers;.
cQuantum yields of open-ring (uc-o) and closed-ring isomers (uo-c);.
dPhotostationary state, respectively.
observed after repeating the above process eight times, indicating excellent fatigue resist-
ance (Figure 2A). The cyclization and cycloreversion quantum yields of 1 were 0.356
(uo-c) and 0.0079 (uc-o), respectively (Table 1). Similar photochromic properties were
obtained when solution of dithienylethenes 2 and 3 in DCM was irradiated with the
same light, as shown in Figures 1B,C and 2B,C and Table 1. The absorption spectral
parameters of dithienylethenes 1–3 in DCM were summarized in Table 1. These data
showed that the aldehyde substituent position had a significant effect on their photo-
chromic properties, mainly including maximum absorption wavelength, molar absorp-
tion coefficients, optical response rate and quantum yields. Among these three isomers,
the absorption maximum of the para-substituted derivative 3c (596 nm) is the longest
in DCM, while that of ortho-substituted derivative 1c (518 nm) is the shortest, which
exhibited 78 nm red-shifts. However, these results were inconsistent with those for
methoxy substituents where the absorption maximum of meta-substituted diarylethene
was the shortest, and that of ortho-substituted one was the longest [20]. As presented in
Table 1, the molar absorption coefficients of ring-closed isomers 1c–3c increased in the
order of meta- < ortho- < para- substitution by the aldehyde group. Furthermore, their
optical response rate was compared, and it was found that the response rate of para-
substituted derivative was the fastest and that of meta- substituted one was the slowest
(Figure 1D). As shown in Table 1, the cyclization quantum yields of dithienylethenes
1–3 were much higher than their corresponding cycloreversion quantum yields. The
cyclization quantum yield of the para-substituted derivative one was the biggest (uo-c
0.526), that of the meta-substituted derivative two is the smallest (uo-c ¼ 0.232).
¼
DFT theoretical calculation
In order to gain an insight into the electronic features and photoreactivity of 1–3, their
optimized molecular geometries and electron densities have been calculated by depend-
ꢃ
ent density functional theory (DFT) in Gaussian 09 B3LYP/6-31G level [30–32]. As
shown in Figure 3, the open-isomers of 1o–3o presented classical antiparallel conform-
ation. Moreover, the HOMO orbital energy of 1o–3o was mainly localized on the cen-
tral dithienylethene unit, while the orbital energy of the LUMO was largely distributed
over the thiophene and formyl substituted benzene moieties due to great effect of elec-
tron deficient formyl group, which exhibited Acceptor-DTE-Acceptor type molecular
skeleton. And higher HOMO-LUMO band gap (3.35 eV for 1o, 3.54 eV for 2o, and
3.53 eV for 3o) for their ring-open isomers was obtained. For the ring-closed isomers
1c–3c, they presented an almost planar conjugated skeleton, and their HOMO and