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solved in deuterochloroform (CDCl3). Its structure was determined
by 1H NMR and 13C NMR spectroscopies. From the results,10 it was
found that it has a symmetric structure similar to the ring-closed
form. The MS (EI) spectral data from this product suggest that
the mass of the yellow product was greater than that of the ring-
closed structure (1c) by the mass of one oxygen atom.
From the chloroform solution in which the large single crystal
with a mass of 33.1 mg was dissolved, a crystal (1b) was obtained
for X-ray crystal structural analysis.11 An ORTEP diagram obtained
by X-ray crystal structural analysis is shown in Fig. 1. The oxygen
atom cross-linked the carbon atoms bearing the two methyl
groups in the benzofuran moieties of the ring-open form. The
cross-linked central ring had a cycloheptadiene structure, which
is unique in this diarylethene series. This compound is a product
of oxidation in air. In addition, the results of elemental analysis
and HR-MS (FAB) also supported this chemical structure. This
structure of the decomposition product is different from that of
1,2-bis(2-methyl-5-phenyl-3-thienyl)perfluorocyclopentene pre-
viously reported.12
Table 1 shows the reaction condition, the yield of 1b, and the
recovery of 1a in decalin. The amount of the decomposition pro-
duct (1b) increased with the time duration of heating at 100 °C.
The yield of 1b reached about 11% after heating in decalin at
100 °C for 72 h. We conducted the reactions in oxygen-free condi-
tion. No decomposition products 1b were present in the reactions
using nitrogen bubbled decalin solution (entry 9 and 10 in Table 1).
The recovery of 1a was a 100% at 100 °C for 72 h.
formalism variant (IEFPCM) for all the calculations. Frequency was
also calculated for the three structures to confirm whether the
structure obtained is energy-minimized at the stationary point.
The absorption spectra of the three structures were obtained by
calculating singlet-excited states using the TD-DFT method in the
range from 200 nm to 600 nm. The difference in the calculated
absorption spectra between wB97XD and CAM-B3LYP was found
to be insignificant (see Supplementary data).
Fig. 3 shows the wavelengths of the absorption maximum and
estimated results corresponding to the ring-opened form (kmax
=
297.62 nm) (1a), the ring-closed form (1c), and the decomposition
product (1b) using CAM-B3LYP as a functional with 6-311+G(d,p)
as the basis set. The correspondence of the magnitude of the molar
extinction coefficient at the absorption maximum of the products
(kmax = 414.82 nm) (1b) to that of the ring-closed form (kmax
=
442.87 nm) (1c) was noted, but the division of the two absorption
bands of 1b cannot be estimated in the visible region. Results of
measurement of X-ray crystal structure and spectroscopic analysis
of one large single crystal show the absence of structural isomers
indicating that transition cannot be simply simulated by calcula-
tion. It may be appropriate to assign the microstructure in the vis-
ible bands to the decomposition product.
The absorption spectra of 1a (ring-opened form), 1c (ring-
closed form), and 1b (decomposition product) in n-hexane are
compared with the molar extinction coefficient on the vertical axis
(Fig. 2). The absorption of the decomposition product (1b) is at the
wavelength slightly shorter than the absorption maximum wave-
length of 469 nm (
(1c). The wavelengths of the absorption maximum were at 454 nm
454, 31,000 MÀ1 cmÀ1) and 432 nm in n-hexane. The decomposi-
e ) of the ring-closed form
469, 14,400 MÀ1 cmÀ1 5
(e
tion product (1b) has a large molar extinction coefficient and two
absorption bands in the visible region.
To determine the difference between 1b and 1c in the absorp-
tion band, their optimized structures were estimated by
calculation.
Time-dependent density functional theory (TD-DFT) calcula-
tions were performed using Gaussian 09W, Rev.D.01.13 We first
obtained optimized structures of 1a, 1b, and 1c using wB97XD or
CAMÀB3LYP as a functional with 6-311+G(d,p) as the basis set.
Recently, the use of long range corrected functionals such as
wB97XD and CAM-B3LYP has produced precise geometries as well
as better prediction of physicochemical properties than that of
B3LYP.14 The effect of solvation in n-hexane was realized using
the polarizable continuum model (PCM) with the integral equation
We synthesized the benzofuran derivative 2a,15 which has phe-
nyl moieties at the reactive carbon atoms to attempt that prevent
from any oxidation. Compound 2a has an absorption maximum at
277 nm (
e
277, 3.42 Â 104 MÀ1 cmÀ1) in n-hexane. Upon irradiation
with visible light, a visible absorption band was observed at 482
nm. It indicated the generation of the ring-closed form 2c (
e
,
482
1.80 Â 104 MÀ1 cmÀ1). The color of 2c disappeared after irradiation
with visible light (k > 440 nm). In a comparative experiment in
decalin at 100 °C for 48 h, no product of the decomposition product
(2b) was observed at all for the compound 2a containing phenyl
substituents at the reaction site (see Supplementary data).
There is a possibility that a decomposition product is formed
with a benzofuran derivative during reactions with an alkyl sub-
stituent at high temperatures in air. However, 1b is hardly pro-
duced by heating at least at 70 °C for 3 h even when 1a is
prepared in a solution. A sample of crystalline 1a obtained 15 years
ago5 by its purification for elemental analysis in a single crystal
state does not contain a yellow decomposition product. Therefore,
1a can be used without any problem if it is stored at room temper-
ature in the dark.
In conclusion, we confirmed by X-ray crystallography the struc-
ture of the decomposition products gradually formed in decalin
solution of 1,2-bis(2-methylbenzofuran-3-yl)perfluorocyclopen-
tene (1a) in air at 100 °C for 24 h or more. The decomposition pro-
duct had a ring-closed form and had a structure in which the
intermediate between the furan moieties were cross-linked at
Fig. 1. ORTEP diagram of 1b. The hydrogen atoms are omitted for clarity.