Communications
In glassy ethanol at 77 K, PET is inhibited as a result of the
mind the discourse in the introductory paragraph, at this stage
the photomediated reaction cycle of the LOV domain comes
into play. If a solution with the chemically activated ensemble
is irradiated with UV light of 254 nm, a strong increase in
BDP fluorescence is noticed. The high efficiency of the
switching process is strikingly evident from a several-100-fold
enhancement of BDP emission and is manifested in tf values
of 4.96 and 5.27 ns for the systems based on 1 and 2. The two
reduced dyads are fully and rapidly converted, and after
turning off the UV-light source, the fluorescence decreases
again to its initial value.
freezing out of solvent reorganization and intramolecular
movement. This interpretation is supported by the results
obtained upon deprotonation of 3 at N3. Such an increase in
electron density at the flavin entails a > 10-fold enhancement
of the BDP emission (Table 2). Dyads 1 and 2, which are
methylated at N3, do not show any spectroscopic changes
upon base addition.
Once the conventional OFF state of the switch was
defined, the next step was to install a control function that
allows this state to be “unlocked”. The versatile redox
chemistry of flavin[6] allows such an activation to be per-
formed chemically. In this experiment and in analogy to thiol-
based natural systems, the spectroscopic changes were
monitored in situ during the chemical reduction of the
flavin moiety with 1,3-propanedithiol[12] and DBU in
MeCN/MeOH (1:1) under an argon atmosphere. The prod-
ucts were the twofold reduced dyads 1red and 2red and
[1,2]dithiolane. As can be seen in Figure 1, the flavin
absorption at 440 nm decreases, whereas the BDP absorption
is not affected, which clearly indicates that the redox process
occurs in the flavin. However, both 1red and 2red are still
weakly fluorescent, with fluorescence lifetimes within the
resolution of the instrument (tf = 3–5 ps). These observations
now mark the chemically controlled OFF state and can be
explained by a reversal of the ET process (Supporting
Information). In the reduced dyads, the electron density at
the flavin is so high that excitation of the BDP triggers a PET
from the flavin to the BDP, reductive PET processes being
well-known for donor-substituted BDPs (Figure 2).[9b]
The reversibility of this reaction is shown in Figure 2,
which indicates that irreversible side reactions do not play a
major role. Most probably, UV irradiation initiates the
formation of a thermally unstable but highly emissive species,
which is accumulated upon continuous irradiation. Dyads 1red
and 2red are then regenerated in a thermal reverse reaction.
Although the real nature of the emitting species could not yet
be analytically determined with methods available to us, the
results strongly suggest that the electron density of the flavin
is considerably lower than in the oxidized state, but higher
than in the fully reduced state. A mono-reduced state can be
excluded as such radicals would also quench the emission.
Thus, we tentatively assume that the light-induced for-
mation of an emissive flavin–thiol adduct in analogy to the
LOV domain photocycle occurs under the prevailing reaction
conditions. The thermal recovery rates reported for LOV
domains are commonly in the range of 0.02 to 0.003 sÀ1,
depending on its type, the medium, and possible protein
assistance.[7,13] These properties suggest that a C4a adduct or a
C4a–C10a cycloadduct might be involved under the present,
more-extreme conditions. Further experiments are currently
underway to elucidate the mechanism in more detail.
In conclusion we have presented novel BDP–flavin dyads
with distinctive electrochemical and optical properties,
including energy- and electron-transfer-modulated emission.
The direction and efficiency of the ET process can be
influenced by various input signals, such as the addition of
base, redox processes, and irradiation with light. These
features distinguish 1 and 2 as potent biomimetic photo-
chemical switches[14] in which the activation state can be
independently controlled and the output emission reversibly
switched.
Now that we were able to switch between an inactive and
an activated OFF state, the last requirement concerned the
input that allows reversible OFF/ON switching. Keeping in
Received: October 20, 2004
Published online: March 8, 2005
Keywords: boron · flavin · fluorescence · molecular switches ·
.
photoreceptors
[1] M. A. van der Horst, K. J. Hellingwerf, Acc. Chem. Res. 2004, 37,
13 – 20.
Figure 2. Reaction scheme of the thermal and photochemical switch-
ing between the non-activated OFF states (1, 2), the activated OFF
states (1red, 2red), and the ON state (reporter state). Inset: Reversible
switching between the activated OFF (mauve) and the ON state
(yellow) of 1red as reflected by the change in emission intensity in
MeCN/MeOH (1:1) during several irradiation cycles with cycle times
of 30 s irradiation and 300 s thermal reverse reaction (c1 =1ꢂ10À6 m).
[2] a) T. Kinoshita, J. Photochem. Photobiol. B 1998, 42, 12 – 19;
b) I. Willner, B. Willner in Molecular Switches (Ed.: B. L.
Feringa), Wiley-VCH, Weinheim, 2001, pp. 165 – 218.
[3] a) O. Pieroni, A. Fissi, N. Angelini, F. Lenci, Acc. Chem. Res.
2001, 34, 9 – 17; b) I. Willner, S. Rubin, React. Polym. 1993, 21,
177 – 186.
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ꢀ 2005 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Angew. Chem. Int. Ed. 2005, 44, 2288 –2291