C O M M U N I C A T I O N S
reversible angular motion of the Cp rings of the ferrocene unit
induced by the photoisomerization of the azobenzene unit.
1H NMR spectroscopy was conducted to investigate a possible
interlocking motion of 1, associated with the pivotal motion around
the ferrocene unit on the isomerization of the azobenzene part. After
1
the trans-to-cis isomerization of 1, the H NMR signals due to
aromatic protons Ha,b (δ 6.99 ppm) and Hc (δ 7.12 ppm) in the
blade phenyl groups (Figure 1) showed downfield shifts by 0.09
and 0.13 ppm, respectively. On the other hand, aromatic signals
due to Hd and He in the handle phenylene groups, observed
respectively at 7.16 and 7.13 ppm for trans-1, showed upfield shifts
by 0.30 and 0.58 ppm, after the isomerization to the cis form. These
spectral change profiles are quite reasonable for the molecular
models of the trans and cis isomers of 1 (Figure 1). Namely, the
two blade phenyl groups in trans-1, which are in close proximity
to each other, become apart from one another on the isomerization
to the cis form. This motion will lead to the lowering of a magnetic
shielding effect from one phenyl group to the other (downfield
shift). On the other hand, the two handle parts in 1 come closer to
each other on the trans-to-cis isomerization of the azobenzene part,
so that each phenylene unit can receive a magnetic effect more
efficiently from the counterpart. Hence, it can now be concluded
that compound 1 undergoes a scissors-like open-close motion upon
light stimuli.
In conclusion, we have succeeded in the molecular design of
the first “light-driven molecular scissors”, where the open-close
motion of the blade parts is interlocked by that of the handle parts
strapped by a photoisomerizable azobenzene unit, due to the pivotal
motion of the connecting ferrocene unit. This work provides a basis
for the development of the next-generation molecular machineries,
which realize further complex motions interlocked by many joint
parts.
Figure 2. (a) Absorption and (b) circular dichroism (CD) spectral changes
of trans-1 (3.5 × 10-5 mol dm-3) in THF at 20 °C upon irradiation with
a UV light (λ ) 350 nm). (c) Light-induced CD intensity change at 285
nm, upon sequential irradiation with a UV light (λ ) 350 nm) for 180 s
(blue areas) and a visible light (λ > 400 nm) for 15 s (yellow areas).
Supporting Information Available: Synthesis of 1-4, details of
crystal structure determination of 4, 1H NMR spectra of 1, and details
of DFT calculation of trans-1 and cis-1 (PDF). X-ray crystallographic
file in CIF format. This material is available free of charge via the
of the azobenzene unit. These spectral changes are typical of those
for the trans-to-cis isomerization of azobenzene derivatives.8 The
molar ratio of trans-1 to cis-1, as determined by HPLC, was 11:89
after photoirradiation. On the other hand, upon irradiation with a
visible light (λ > 400 nm) for 15 s at 20 °C, a backward
isomerization took place to furnish the cis/trans isomer ratio of
54:46. Thus, the azobenzene unit in compound 1 can reversibly
isomerize in response to UV and visible lights.
The enantiomers of trans-1 displayed characteristic CD spectra.
For example, [CD(-)280]-trans-1 showed a negative Cotton effect
at 272.5 nm and positive Cotton effects at 256.0 and 315.5 nm
(Figure 2b). The trans-to-cis isomerization of [CD(-)280]-trans-
1, upon UV-irradiation (λ ) 350 nm) for 180 s, was accompanied
by a CD spectral change at 240-300 nm due to the major
absorption of the tetraarylferrocene unit. On the other hand, upon
irradiation with visible light, (λ > 400 nm), a reverse CD spectral
change occurred, where the system quickly reached a photo-
stationary state in 15 s. On sequential irradiation with UV and
visible lights in an alternating manner, the sign of the Cotton effect,
e.g., at 280-290 nm was inversed from negative to positive and
then from positive to negative (Figure 2c). These results suggest a
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