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potentials of fast photochromic molecules into full-color
holographic displays12 eventually for commercially available
televisions, wavelength-selective high security systems, and
color-selective filters for detectors to avoid instantaneous
saturations of light. In addition to industrial applications, fast
photochromic molecules which respond to visible light can be
used as a trigger pulse to induce unfolding of proteins,13,14
motions of protein motors,15 and isomerization of DNAs,16,17
and they offer a possibility to observe dynamic conformation
changes in real time.
In this study, we overcome these issues with sustaining fast
photochromism and high durability by flipping both imidazole
rings of pseudogem-bisDPI[2.2]PC. The alteration in the
relative configuration of the imidazole rings suppresses the
broad absorption band due to the radical−radical interaction.
When we call pseudogem-bisDPI[2.2]PC as the head-to-head
form (HH), in which the 2-position of both imidazole rings
binds to a [2.2]paracyclophane (PC) moiety, we synthesized
the head-to-tail form of pseudogem-bisDPI[2.2]PC (HT,
Scheme 1b) and the tail-to-tail form of pseudogem-bisDPI[2.2]-
PC (TT, Scheme 1c), in which the 4-position of one of the
imidazole ring or both imidazole rings bind to the [2.2]PC
moiety. The 2-position of the imidazole ring of the tail-to-tail
form is easily substituted by using aldehyde derivatives, and the
substituent can drastically modulate both steady-state and
transient absorption spectra. The aldehyde derivatives are
widely available in various companies and are much easier to
synthesize as compared to diketone derivatives, which are
necessary to substitute the head-to-head form. As a
demonstration, we attached two pyrenes to the 2-position of
both imidazole rings of the tail-to-tail form of the bridged
imidazole dimer (Py-TT, Scheme 1d) and showed how the
spectra drastically changes. Fast photochromic molecules with
the wavelength tunability and the visible sensitivity have
potentials to develop novel practical applications and to
establish new academic fields.
Scheme 1 illustrates the photochromism of HH, HT, TT,
and Py-TT, respectively. The process of their photochromism
is identical irrespective of the configuration of the imidazole
rings. Upon UV irradiation, the radical pair, which is the origin
of the coloration, is generated by the C−N bond cleavage, and
two radicals thermally recombine and recreate the C−N bond.
The steady-state absorption spectra of HT and TT slightly shift
to the red region as compared to that of HH, which gradually
increases from ∼370 nm (Figures S21 and S22), but their
spectral shapes are generally similar. Figure 1 shows transient
absorption spectra of HH, HT, and TT. The vertical lines
indicate the theoretical spectra for the colored species obtained
by the TDDFT calculations (UMPW1PW91/6-31+G(d,p)//
UM052X/6-31G(d)). The insets show ORTEP representations
of their molecular structures obtained by X-ray crystallographic
analysis. As we see from the structures, while the C−N bonds
of HH and HT bind the 1- and 2′-position of the imidazole
rings (1,2′-isomers), TT is the 1,4′-isomer. HT is intrinsically
different from the head-to-tail form of the naphthalene-bridged
imidazole dimer, which is the 1,4′-isomer.18 As shown in Figure
1a, we observe a strong absorption band around 400 nm and a
broad absorption band over the visible region for HH. The
TDDFT calculations indicate that two bands at ∼400 and 500−
600 nm are attributed to the imidazolyl radical, and the band
over 600 nm is attributed to the radical−radical interactions,
which are supported by our previous report.19 The transient
absorption spectrum of HT shows the similar spectrum to that
Figure 1. Transient absorption spectra of (a) HH, (b) HT, and (c)
TT in degassed benzene (excitation wavelength, 355 nm; pulse width,
5 ns; power 4 mJ/pulse; the concentrations of HH, HT and TT are
2.1 × 10−4, 2.2 × 10−4 and 1.1 × 10−4 M, respectively). Vertical lines
indicate the theoretical spectra for the colored species of each
molecule (TDDFT UMPW1PW91/6-31+G(d,p)//UM052X/6-
31G(d)). Insets show ORTEP representations of the molecular
structures obtained by X-ray crystallographic analysis.
of HH, but the absorption band derived from the radical−
radical interaction decreases and shifts to the red region (Figure
1b). The decrease and the shift are more pronounced in the
transient absorption spectrum of TT, while the absorption band
due to the imidazolyl radical is similar to each other (Figure
1c). The transient absorption spectrum of TT has little
absorption around the red region, and only the absorption band
due to the imidazolyl radical is observed because of the reduced
overlap integral of the wave function. The decrease in the
radical−radical interaction is caused by the increase in the
distance and the displacement between two imidazole rings.
The optimized geometries of the colored species of HH, HT,
and TT are shown in Figures S39, S43, and S47, respectively.
The absorption band derived from the radical−radical
interaction is red-shifted in the order corresponding to HH,
HT, and TT. These absorption bands are mainly attributed to
the HOMO−LUMO transition from the orbital localized at an
imidazole ring to the orbital localized at the other imidazole
ring.
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dx.doi.org/10.1021/ja501028v | J. Am. Chem. Soc. 2014, 136, 3796−3799