Fabien Kohl1, Aaron Gerwien2, Frank Hampel1, Peter Mayer2, Henry Dube1. 1. Department of Chemistry and Pharmacy, Friedrich-Alexander Universität Erlangen-Nürnberg, Nikolaus-Fiebiger-Str. 10, 91058 Erlangen, Germany. 2. Department of Chemistry and Center for Integrated Protein Science (CIPSM), Ludwig-Maximilians Universität München, Butenandtstr. 5-13, 81377 Munich, Germany.
Abstract
Molecular photoswitches that offer simultaneous precise control over geometrical and electronic changes are rare yet highly sought tools for the development of responsive nanosystems. Here we present such an advantageous combination of property control within a novel multiphotoswitch architecture. Hemithioindigo-based trioxobicyclononadiene (HTI-TOND) offers a rigid three-dimensional molecular structure that undergoes different exotic rearrangement reactions upon photochemical and thermal signaling. Three to four different states with distinct geometric and electronic properties can be accessed reversibly in high yields within this molecular framework. Thus, a highly promising and unique switching tool has become available to instill the next level of addressability at the smallest scales.
Molecular photoswitches that offer simultaneous precise control over geometrical and electronic changes are rare yet highly sought tools for the development of responsive nanosystems. Here we present such an advantageous combination of property control within a novel multiphotoswitch architecture. Hemithioindigo-based trioxobicyclononadiene (HTI-TOND) offers a rigid three-dimensional molecular structure that undergoes different exotic rearrangement reactions upon photochemical and thermal signaling. Three to four different states with distinct geometric and electronic properties can be accessed reversibly in high yields within this molecular framework. Thus, a highly promising and unique switching tool has become available to instill the next level of addressability at the smallest scales.
Molecular switches are central
building blocks in functional chemical systems that allow the introduction
and control of precise changes at the smallest scales of matter. Photoswitches
in particular offer distinct advantages because they use light as
a fast and waste-free signal to affect the switching processes. For
these reasons, photoswitches have risen to great prominence, and myriads
of applications have been reported in which they have been employed
as indispensable bases of responsive smart chemical systems.[1−11] Many different types of photoswitches are being explored presently,
which can roughly be divided into two classes, enabling either strong
geometric or strong electronic changes upon switching. In the first
case, the photochromism and electronic changes are typically not very
large, with azobenzenes[12] and stilbenes[13,14] being classical examples and imines,[15,16] hydrazones,[17−19] and indigoid photoswitches[7,20] representing later
additions. In the second case, geometry changes are oftentimes subtle,
as can be seen for example in diarylethenes[21] and dihydropyrans.[22−25] Nevertheless, there are few examples in which both properties can
be combined to some extent, and larger geometric changes are matched
with severe electronic changes, such as in spiropyrans or the recently
introduced Stenhouse dyes.[26−28] Here strong photochromism and
electronic changes are found in conjunction with distinct geometry
changes. Such a combination is beneficial for virtually any application
since both electronic changes (conjugation, polarity, photochromism,
etc.) and geometry changes (proximity alterations, spatial distribution
of functional groups, etc.) can then be controlled with the highest
precision.In this work, we present an entirely unexplored type
of fundamental
photoswitch, hemithioindigo[7,20]-based trioxobicyclononadiene
(HTI-TOND) 1 (Figure ). HTI-TOND enables
the desirable combination of concomitant geometry
and electronic changes within a distinct molecular framework. It allows
alteration between up to four different stable states A to D instead of the usual two states found in most
fundamental photoswitches. The TOND state is a highly rigid 3D molecular
structure offering precise placement of functional groups in space.
The other states are more flexible and in addition are differently
conjugated, offering distinct electronic communication between molecular
parts. The photoswitching processes employ two exotic reactions, a
rare “forbidden” hetero-Diels–Alder/retro-Diels–Alder
reaction (TOND A to C/D conversions)
and an oxygen rearrangement reaction (B to C/D conversions), which are now introduced as novel mechanistic
tools into the realm of photoswitching. In addition, a thermal oxygen-rearrangement
reaction leading from TOND A to isomer B is also uncovered.
Figure 1
HTI-TOND 1 enabling switching between four
different
states A (racemic rigid TOND structure), B, C, and D with distinct geometric and
electronic properties. Schematic structures, photo- or thermally induced
net interconversions, and the corresponding structures in the crystalline
state are shown alongside photographs of pure isomer solutions in
toluene.
HTI-TOND 1 enabling switching between four
different
states A (racemic rigid TOND structure), B, C, and D with distinct geometric and
electronic properties. Schematic structures, photo- or thermally induced
net interconversions, and the corresponding structures in the crystalline
state are shown alongside photographs of pure isomer solutions in
toluene.TOND-like structures are quite
rare but are found in some natural
products produced by fungi and bacteria.[29−33] The simple methylated derivative was discovered in
complexation with platinum in 1965 by Gibson et al.,[34] and its resolution was reported in 1977 by de Renzi et
al.[35] Further TOND motifs have later been
explored for synthetic accessibility[36−39] and applications in, e.g., supramolecular
chemistry,[40−44] mainly by Kollenz and co-workers but also by others.[45−47] To the best of our knowledge, no photochemistry has been reported
to date. The HTI-TOND motif presented herein provides a hitherto not
described aryl-substituted version of the TOND structure, enabling
further functionalization on the periphery and in different spatial
quadrants.HTI-TOND system 1 was synthesized in
four high-yielding
steps that represent an alteration of a previously reported protocol
for synthesizing highly substituted HTIs[48] (Scheme ). Starting
from commercially available thiosalicylic acid and 2-bromo-4′-methoxyacetophenone,
a nucleophilic substitution reaction affords the corresponding thioether 2 quantitatively. Intramolecular condensation under mildly
basic conditions leads to hydroxythiophene derivative 3 in 79% yield, which subsequently is transformed into chlorinated
HTI 4 in 96% yield after reaction with thionyl chloride.
When precursors 3 and 4 are combined in
the presence of K3PO4 at elevated temperatures,
photoswitch 1 is obtained in 78% overall yield either
as sole HTI-TOND A or as an isomeric mixture of 38% HTI-TOND A and 40% C, depending on the reaction duration.
After application of different heating or irradiation steps, the four
isomers of 1 (A to D) could
be accumulated to varying degrees. Separation of the isomers using
HPLC was possible because of their sufficiently high thermal stabilities.
Identification and spectral assignment was facilitated by X-ray diffraction
analysis in the crystalline state for all four isomers (see Figure ).
Scheme 1
Simple and High-Yielding
Four-Step Synthesis of HTI-TOND 1
The thermal behavior of the HTI-TOND system was first
examined
at different temperatures to establish its ground-state energy profile
at the common temperature of 22 °C (Figure ). The thermodynamically most stable state
was found to be isomer B, which is obtained after prolonged
heating to temperatures above 100 °C of, e.g., isomer A in toluene-d8 solution. This reaction
represents an unusual oxygen-rearrangement reaction in which not only
two oxygen–carbon bonds are broken within the TOND structure
but also new oxygen–carbon connectivity is established. An
in-depth mechanistic investigation of this reaction will be the topic
of a future dissemination. Heating a solution of either isomer C or D over prolonged times above 100 °C
also leads to full conversion to pure isomer B. However,
when the temperature is lowered, thermal isomer conversions become
clearer. Starting from pure isomer C, HTI-TOND A is accumulated first as the direct isomerization product
at 60 to 90 °C. When pure isomer D is heated, HTI-TOND A is also the direct isomerization product—even at
ambient temperatures where no further thermal isomerization to B takes place. At the same time, a small amount of isomer C is also formed from D. Because of the different
activation energies for thermal isomerizations, HTI-TOND A or isomer B can be accumulated in high yields in thermal
steps from isomers C and D if the temperature
is controlled well. The corresponding Gibbs energies of activation
ΔG⧧ as determined from kinetic
analysis are given in Figure d. Since no thermal equilibria are established and isomer B is formed as the sole product after prolonged heating, only
lower limits for the energy differences ΔG between
isomers can be given by assuming 5% of a remaining isomer is not detected
in the experiments. We further tested the effect of acid addition
on the thermal behavior of 1. After addition of trifluoroacetic
acid (TFA) to a solution of pure isomer C in toluene-d8 solution, a significant acceleration of the
thermal isomerization to exclusively HTI-TOND A took
place even at ambient temperatures. Therefore, thermal reactions in
the presence or absence of acid can be used to gain improved control
to access the two most stable states A and B.
Figure 2
Thermal isomerization reactions of HTI-TOND system 1 and corresponding ground-state energy profile. (a–c) 1H NMR spectra (400 MHz, toluene-d8) showing thermal conversions of isomer HTI-TOND A at
100 °C, isomer C at 60 °C, and isomer D at 22 °C, respectively. Marked signals correspond to
the OMe groups. (d) Experimental (red, all values correspond to 22
°C) and theoretical (violet) ground-state energy profile of 1.
Thermal isomerization reactions of HTI-TOND system 1 and corresponding ground-state energy profile. (a–c) 1H NMR spectra (400 MHz, toluene-d8) showing thermal conversions of isomer HTI-TOND A at
100 °C, isomer C at 60 °C, and isomer D at 22 °C, respectively. Marked signals correspond to
the OMe groups. (d) Experimental (red, all values correspond to 22
°C) and theoretical (violet) ground-state energy profile of 1.The experimental findings are
generally in good agreement with
the theoretical description conducted at the MPWB1K/6-311G(d,p)/gd3bj
level of theory, as shown in Figure d (for further details, see the Supporting Information).The photochemistry of the HTI-TOND
system 1 was investigated
next by studying the photoreactions of the individual isomers separately
(Figure ). As depicted
in Figure a, isomers A, B, and C/D show
distinctly different molar absorptions, which are well-reproduced
by the theoretical description (see the Supporting Information). The absorptions of isomers C and D appear to be most red-shifted but are not well-distinct
from each other, which prevents effective photoswitching between just
these two isomers. The absorption of HTI-TOND A resides
only in the UV part of the absorption spectrum, and thus, photochemistry
needs to invoke light of 300 nm. Irradiation at that wavelength in
toluene(-d8) solution at −25 °C
(to exclude thermal reactions of D) leads to the appearance
of the spectral hallmarks of isomers C and D in the absorption and 1H NMR spectra. In the photostationary
state (pss), a mixture comprising 19% remaining HTI-TOND A and a total of 81% isomers C (50%, dominating species
in solution) and D (31%) is formed. It is thus established
that photoirradiation of HTI-TOND A with UV light leads
to a rather exotic photochemical retro-hetero-Diels–Alder (RHDA)
reaction that opens the TOND structure, yielding an intense yellow
color of the solution. This photoreaction also delivers a different
isomer than the thermal reaction of HTI-TOND A, which
establishes the latter as the branching point for the switching capacity
of 1.
Figure 3
Photoisomerization and switching reactions of HTI-TOND
system 1. (a) Molar absorptions of individual isomers A, B, C, and D of 1. (b) 1H NMR (400 MHz, toluene-d8) spectra showing photoconversions between individual
isomers
of 1 (MeO signals are shown). (c) Cycle experiment followed
by 1H NMR spectroscopy (400 MHz, toluene-d8) in which isomers of 1 are converted in
the sequence A → C/D → A → B → A.
Photoisomerization and switching reactions of HTI-TOND
system 1. (a) Molar absorptions of individual isomers A, B, C, and D of 1. (b) 1H NMR (400 MHz, toluene-d8) spectra showing photoconversions between individual
isomers
of 1 (MeO signals are shown). (c) Cycle experiment followed
by 1H NMR spectroscopy (400 MHz, toluene-d8) in which isomers of 1 are converted in
the sequence A → C/D → A → B → A.Isomer B possesses
an absorption that reaches the
400 nm mark with its tail. It can thus be irradiated with light of
longer wavelengths (e.g., 365 nm in toluene(-d8)) at different temperatures, leading to population of isomers C and D in roughly equal amounts first and then
to almost complete conversion to HTI-TOND A after prolonged
irradiation times. Low-temperature irradiation of B shows
that this behavior is due solely to photoconversions, including a
less efficient photoreaction from B to A, resulting in a pss with up to 97% A accumulated. The
dominating photochemical reaction from B to C/D represents again a rather exotic oxygen-rearrangement
reaction, which also differs from the corresponding thermal rearrangement
leading from HTI-TOND A to B. The mechanism
is again not clarified at this point and is currently under investigation
in our laboratory. When toluene(-d8) solutions
of pure isomer C are irradiated at a wavelength of 300
or 365 nm at different temperatures, isomer D is populated
initially as the product of Z/E photoisomerization,
but conversion to HTI-TOND A over prolonged irradiation
times is also observed. Likewise, irradiation of isomer D leads to almost complete conversion to isomer A after
prolonged irradiation times with 365 nm or longer-wavelength light.Taking the photochemistry of 1 together, irradiation
of isomer B with 365 nm light populates isomer A almost quantitatively. Isomers C and D can be accumulated in up to 81% yield after irradiation
of HTI-TOND A with 300 nm light and thus serve as a thermally
stable third state. When in turn isomers C and D are irradiated with 365 nm light, they readily convert back
to A photochemically. Some degradation is observed in
the photoreactions (see the Supporting Information), but in the presence of acid the overall switching processes are
facilitated and proceed more rapidly.Overall, it is thus possible
to access three different states of 1 in high percentages
and convert them reversibly into each
other using light of different wavelengths and heat as signals. The
fourth isomer D cannot be enriched to the degree of being
the dominant species in solution at present. However, up to 30% D can be obtained by irradiation of isomer A at
low temperatures. HTI-TOND isomer A serves as the branching
point, from which isomers B and C/D can be obtained in high yields either thermally or photochemically,
respectively. To illustrate, we have conducted a cycle experiment
interconverting the isomers in the sequence A → C/D → A → B → A (Figure c). Additionally, the interconversion sequence A → B → A was conducted
four times (see the Supporting Information), evidencing multiple switching cycle capacity.In summary,
we have presented a unique molecular photoswitch that
allows multistate switching in different sequences by a combination
of light and heating signals. During switching the rigidity and electronic
character of the molecular architecture are altered significantly,
leading from colorless to deep-yellow solutions. Unusual RHDA and
rearrangement photo- and thermal reactions are employed for the isomerization
processes, which now enter the stage of photoswitching together with
a unique molecular 3D structure as a novel motif for responsive nanosystems.
We believe that this photoswitching system offers highly interesting
and distinctive possibilities for responsive molecular functions in
all chemistry-related fields. Applications as well as mechanistic
elucidations are currently under investigation in our laboratory.
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