Visible-Light Photochromism in Diethynylethenes
COMMUNICATION
Figure 4. Time-course UV/Vis spectral change of E-4 in toluene upon ir-
radiation with l=500 nm light. The inset shows a time-course 1H NMR
spectral change in [D8]toluene under the same condition.
reaction was traced by time-course UV/Vis (Figure 4) and
1H NMR spectral changes (inset of Figure 4). The former
possessed an isosbestic point, which ensured the absence of
side reactions. Irradiation at l=500 nm to E-4 gave rise to
a nearly quantitative conversion to Z-4: the proportion of
the Z-isomer in the photostationary state (PS) reached
1
>99%, judging from the integral ratio in the H NMR spec-
Figure 5. Cyclic voltammograms (black solid line) of a) E-4 and b) Z-4 in
nBu4NBF4-dichloromethane (0.1m) and its simulation (red circles). E0’(1),
E0’(2), and DE0’ are extracted from the simulation.
trum. Both E and Z isomers were thermally stable, because
the spectra did not change at all when the solution samples
were stored in the dark. We note that the E/Z ratio at the
PS could be tuned reversibly by changing the excitation
wavelength (Scheme 2). For example, upon irradiation at
l=400 nm, the proportion of the Z isomer in the PS was re-
duced to 71% (Figures S7 and S8 in the Supporting Infor-
mation).
The E/Z photoisomerization-quantum yields in 4 upon ir-
radiation with l=400 nm light was calculated by the proce-
dure reported by Zimmerman et al.[9] Figures S9 and S10 in
the Supporting Information display the experimental plot
and equations, respectively. This calculation gave FE!Z and
FZ!E of 0.30 and 0.10, thereby affording Ftotal of 0.40.
Therefore, the Ftotal of E/Z-4 was far greater than that of
E/Z-1 (Ftotal =1.1ꢀ10ꢀ5) and 5.3 times greater than that of
E/Z-2 (Ftotal =0.075).
the Supporting Information). According to the simulation,
E0’(1) and E0’(2) are 496 and 541 mV for E-4, and 501 and
532 mV for Z-4 (Figure 5). The separation of the formal po-
tentials between the two chemically equivalent redox sites,
DE0’ =E0’(2)ꢀE0’(1), can be a good indicator for electronic
communication.[7] Value DE0’ is greater in E-4 (45 mV) than
in Z-4 (31 mV); therefore, E-4 should possess more intense
electronic communication in the monocationic MV state.
We note DE0’ is modulated by other factors, such as Cou-
lomb repulsion, statistical term, inductive effect, and so
on.[10] However, these sidebar factors should be nearly iden-
tical in E-4 and Z-4, except for the Coulomb factor. This
through-space interaction should be more intense in the Z
ꢀ
Pursuit of solid-state photoisomerization in E/Z-3 and
E/Z-4 was unsuccessful. Instead, both E-3 and E-4 exhibited
strong fluorescence even in the solid state (Figure S11 in the
Supporting Information), which might be appreciated in
solid-phase applications, such as electroluminescence devi-
ces.
To quantify the modulation of electronic communication
in the one-electron oxidized MV state upon the photoisome-
rization, cyclic voltammetry was conducted for both E-4 and
Z-4 (Figure 5). Both isomers underwent two reversible and
close one-electron oxidations with respect to the two NPC
moieties. Therefore, simulation of the voltammograms was
conducted to acquire the formal potentials of the two oxida-
tions of the two NPCs, E0’(1) and E0’(2). The result of the
simulations is also shown in Figure 5 as red circles (for the
detail parameters of the simulation, see Tables S3 and S4 in
form (8.4 ꢂ for the N N bond length, from the single-crys-
tal X-ray structure of Z-4) than in the E form (17.2 ꢂ, from
that of E-4). Nevertheless, the greater DE0’ was observed in
E-4; hence, one can conclude that the electronic communi-
cation is truly more intense in E-4 than in Z-4. The weaker
electronic communication in Z-4 should originate from the
steric repulsion between the methyl ester moieties (Fig-
ures 1, 2, S4, and S5 in the Supporting Information), which
disturbs the p conjugation between the two NPCs,[4b] as evi-
denced by the blueshift of the ICT band in the Z form (Fig-
ures 3, S6 in the Supporting Information, and Table 1).
We note that the methoxy group at the 3- and 3’-positions
in E/Z-4 is essential for the reversible electrochemical be-
havior: without methoxy substituents, E-3 underwent irre-
versible oxidations (data not shown). Instead, oxidative elec-
tropolymerization was observed.[11] Thus, when an ITO plate
Chem. Eur. J. 2012, 00, 0 – 0
ꢁ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
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