Vincenzo Balzani*a, Paola Ceronia, Alberto Credia, Marcos Gómez-Lópezb, Christoph Hamersb, J. Fraser Stoddart*c and Reinhard Wolfb
aDipartimento di Chimica “G. Ciamician”, Uniersità di Bologna, ia Selmi 2, 40126, Bologna, Italy. E-mail: vbalzani@ciam.unibo.it
bSchool of Chemistry, The Uniersity of Birmingham, Edgbaston, Birmingham, UK B15 2TT
cDepartment of Chemistry and Biochemistry, Uniersity of California, 405 Hilgard Aenue, Los Angeles, California 90095-1569, USA. E-mail: stoddart@chem.ucla.edu
First published on 15th December 2000
A scorpion-like pseudorotaxane (1·H2+), composed of a macrocyclic polyether containing a 1,5-dioxynaphthalene (1,5-DON) and a 1,3-dioxybenzene (1,3-DOB) electron-donor unit, the latter bearing a 4,4′-bipyridinium electron-acceptor tail, underwent threading/dethreading motions under control of (i) solvent polarity and (ii) solution acidity. Furthermore, the complexation of 1 ·H2+ with the trans-1,2-bis(1-benzyl-4-pyridinio)ethylene electron acceptor can be acid/base controlled. The spectroscopic properties of a related macrobicyclic compound 24+ (comprised of an electron-donor and an electron-acceptor macrocycle that share a benzene ring) have also been investigated. The results obtained for 24+ are consistent with the presence of intramolecular self-complexed species where the electron-donor macrocycle is threaded through the electron-acceptor one. Electrochemical experiments confirm the self-complexing structures of 1·H2+ and 24+. It seems likely that both compounds undergo decomplexation upon electrochemical stimulation.
Conventional pseudorotaxanes4 are made of two covalently disconnected components, namely a macrocycle and a thread (Fig. 1a), which contain complementary recognition sites. The threading and dethreading motions can be controlled by an external stimulus capable of switching on/off one of the recognition sites.5 In the dethreaded state each of the two components, the macrocycle and the thread, are free to move independently in solution. Such a “disordered” situation can nevertheless lead to well defined properties for the supramolecular system, e.g. all the free threads are luminescent whereas the threaded ones are not.5,6 Therefore, the threading/dethreading process can exhibit binary logic behavior. It has indeed been shown that suitably designed pseudorotaxanes can perform as molecular-level logic gates.6
Fig. 1 Schematic representations of (a) a conventional pseudorotaxane and (b) a self-complexing molecule in which a macrocycle is linked by a covalent tether to a tail containing a recognition unit. |
From the machine-like viewpoint, however, the molecular level structure and the movement of the component parts should be spatially well defined. For pseudorotaxane-type systems this goal can be reached in a molecular context by connecting7 (Fig. 1b) the macrocycle and the thread by a covalent tether. The result is a self-complementary molecule.8
Several examples of compounds consisting of a macrocyclic head and a tail that contain complementary recognition sites have recently been studied.7,9–11 In this paper we report the results of an investigation on the dethreading/rethreading motions of compound 1·H2+ and on the self-complexation of the related macrobicyclic compound 24+, which is comprised of electron-donor and electron-acceptor macrocycles sharing a benzene ring (Fig. 2).
Fig. 2 Structural formulae of the investigated compounds 1·H2+ and 24+, as well as of the t-BBPE2+ species that has been used in the experiment described in Fig. 8. |
Fig. 3 Structural formulas of the model compounds 3 ·H24+, 4, 54+ and 64+ for the electroactive units of compounds 1·H2+ and 24+. |
In very dilute solutions (3 × 10−5 mol L−1) the absorption spectrum of compound 1 ·H2+ in MeCN at 298 K (Fig. 4, curve a) shows only a very weak tail (ε<70 L mol−1 cm−1) in the visible region and it is very similar to the sum of the spectra of its chromophoric units, namely 1,5-DON, 1,3-DOB, and 4,4′-bipyridinium. On increasing concentration, however, the structure of the 1,5-DON band is lost, the intensity of the tail in the visible spectral region increases and the solution becomes colored. For a 2 × 10−3 mol L−1 solution a band with maximum at 480 nm (ε = 150 L mol−1 cm−1) can be observed (Fig. 4, curve b).
Fig. 4 Absorption spectrum at 298 K of compound 1 ·H2+ in: (a) 3 × 10−5 mol L−1 MeCN solution; (b) 2 × 10−3 mol L−1 MeCN solution; (c) 3 × 10−5 mol L−1 CH2Cl2 solution. |
The absorption spectrum of compound 1·H2+ in CH2Cl2 solution is similar, but not identical, to that observed in concentrated MeCN solution (Fig. 4, curve c). In this case, however, the spectrum does not depend on the concentration. The most important feature is the presence of an absorption band in the visible region (λmax = 510 nm, ε = 300 L mol−1 cm−1), responsible for the pink color of the solution.
The different results obtained for MeCN and CH2Cl2 solutions can be accounted for as follows. The absorption bands observed in the visible region are typical5c,7a,12 of the charge-transfer (CT) interaction between bipyridinium dications and 1,5-DON. In CH2Cl2 the dicationic bipyridinium unit is self-complexed with the macrocyclic part of the molecule, whose oxygen atoms offer a much more favorable environment than the non-polar solvent molecules (1,1′-dimethyl-4,4′-bipyridinium is highly insoluble in CH2Cl2). Although intermolecular complexation is possible, evidence for intramolecular complexation is given by the fact that the absorption spectrum does not change with concentration.17 Inspection of CPK (Corey-Pauling-Koltun) space-filling molecular models shows that the bipyridinium tail can easily be accommodated inside the macrocycle. A threaded structure (Fig. 5a) seems therefore more likely than a side-on one (Fig. 5b) because the former facilitates formation of additional [C–H···O] hydrogen bonds between the α bipyridinium hydrogen atoms and some of the polyether oxygen atoms.18
Fig. 5 Cartoons representing the threaded (a), side-on (b) and dethreaded (c) conformations of compound 1·H2+. |
In MeCN the dicationic bipyridinium moiety is well solvated by the polar solvent molecules, so that, in dilute solutions, the more stable isomer of compound 1·H2+ is the decomplexed one (Fig. 5c). This suggestion is supported by the low values of association constants between aromatic crown ethers and 1,1′-dimethyl-4,4′-bipyridinium in MeCN solution.19 The weak absorption tail in the visible region observed under such conditions (Fig. 4, curve a) can be assigned to a through-bond CT interaction between the 1,3-DOB moiety of the macrocycle and the appended bipyridinium unit. As the concentration increases, however, intermolecular complexation takes place and a CT band arising from the interaction between the 1,5-DON and bipyridinium units appears.
Evidence for the presence of decomplexed species in dilute MeCN and self-complexed ones in CH2Cl2 is also provided by the fluorescence measurements. Although the intense fluorescence band characteristic of the 1,5-DON unit (λmax = 328 nm, τ = 7.5 ns in aerated MeCN)13 is strongly quenched,20,21 in both solvents, in CH2Cl2 solution the fluorescence intensity quenching is ten times larger than that observed in dilute MeCN solution. This observation suggests that, in CH2Cl2 solution, compound 1·H2+ adopts a conformation that maximizes the quenching of the potentially luminescent 1,5-DON unit, as would be the case when the bipyridinium tail is threaded (Fig. 5a) in the crown ether ring.22 Addition of MeCN to a 5 × 10−5 mol L−1 CH2Cl2 solution of 1·H2+ causes the disappearance of the visible absorption band and an increase in the fluorescence intensity (Fig. 6), showing that the larger fluorescence quenching observed in CH2Cl2 solution is indeed related to the conformation which is responsible for the presence of the CT absorption band in the visible region. Concentrated (1 × 10−3 mol L−1) MeCN solutions of 1·H2+ show a much stronger fluorescence quenching20 than dilute (2 × 10−5 mol L−1) ones, as expected because of the intermolecular complexation (see above).
Fig. 6 Changes in the absorbance at 510 nm (●) and in the fluorescence intensity at 345 nm (λex = 295 nm) (□) upon addition of MeCN to a 5 × 10−5 mol L−1 CH2Cl2 solution of compound 1·H2+ at 298 K. |
In conclusion, the conformation of compound 1 ·H2+ is solvent dependent:23 the dethreaded conformation is the more abundant one in very dilute solutions of the polar solvent MeCN and the self-threaded18 one is preferred in the non-polar solvent CH2Cl2. Since the conformational change is accompanied by a visible color change and by a change in the fluorescence intensity, 1·H2+ can be viewed as an optical sensor for solvent polarity.
These results can be accounted for as shown in Fig. 7. Upon addition of a base the terminal pyridinium ring of compound 1·H2+ undergoes deprotonation, so that the tail becomes a monocationic 4-pyridyl(4-pyridinium) unit. Since a pyridyl unit is not a good electron acceptor, while a pyridinium unit is, this tail is a much poorer electron acceptor than the protonated tail, so that the original CT interaction with the electron donor macrocycle is disabled. At the same time deprotonation makes the tail much more soluble in the non-polar CH2Cl2 solvent. As a consequence, deprotonation causes dethreading, while addition of acid directs the system back to the threaded conformation.18,24
Fig. 7 Base/acid-driven dethreading/rethreading of compound 1·H2+. |
The absorption spectrum of a CH2Cl2 solution containing 3.2 × 10−4 mol L−1 compound 1·H2+ and 9 × 10−6 mol L−1 t-BBPE2+ (whose solubility in CH2Cl2 is very low) matches exactly the sum of the spectra of the isolated components in the same concentration. After addition of 6.4 × 10−4 mol L−1 tributylamine the absorption spectrum becomes different from the sum of the spectra of the components; in particular, a decrease in the intensity of the absorption bands characteristic of the 1,5-DON unit (311 and 326 nm) and of t-BBPE2+ (340–350 nm), and the appearance of an absorption tail in the 350–380 nm region, are observed. These changes are the same as those observed in the absorption spectrum of the solution containing 1,5DN38C10 and t-BBPE2+. Owing to the lack of suitable luminescence signals,25 it is difficult to assess the amount of t-BBPE2+ threaded through 1+. A rough calculation done on the basis of the absorption tail intensity at 370 nm, compared with that of the 1,5DN38C10/t-BBPE2+ system, suggests that t-BBPE2+ is quantitatively engaged by 1+. Evidence of strong complexation comes also from a comparison of low-temperature emission spectra. At 77 K, t-BBPE2+ shows an intense and structured fluorescence band that can no longer be seen in frozen solutions which also contain, besides 9 × 10−6 mol L−1 t-BBPE2+, 3.2 × 10−4 mol L−11·H2+ and 6.4 × 10−4 mol L−1 tributylamine. This behavior can be explained by the fact that the fluorescence is quenched by low-lying CT levels when t-BBPE2+ is encapsulated within the macrocyclic crown ether. Although it is difficult to push this comparison to a fully quantitative level, there is evidence that a large amount of t-BBPE2+ is complexed by 1+.
The results can be rationalized as schematized in Fig. 8. t-BBPE2+ is a poorer electron acceptor than the 4,4′-bipyridinium unit;12 moreover, the latter is entropically advantaged, as it is covalently linked to the host crown ether. Thus, t-BBPE2+ cannot dethread compound 1·H2+. When tributylamine is added 1·H2+ undergoes deprotonation and then dethreading (see above) so that the external guest can enter the open macrocyclic cavity. This process can be reversed by addition of 2.5 × 10−3 mol L−1 CF3CO2H: the terminal pyridine unit of 1+ is protonated and the 1 ·H2+ species undergoes self-threading, pushing t-BBPE2+ out of the macrocycle cavity. In conclusion, amines can open and protons can close the ‘door’ of the macrocyclic cavity of 1·H2+, thereby allowing or preventing the threading of an external guest.
Fig. 8 Base/acid control of the complexation of t-BBPE2+ by compound 1+. |
Compound | Solvent | E/V s. SCEa | |||
---|---|---|---|---|---|
a Halfwave potential values (E1/2), unless otherwise noted.b Chemically irreversible process; Ep value at scan rate of 0.2 V s−1.c Two-electron transfer process.d After addition of tributylamine in a stoichiometric amount with respect to the number of protonated 4-pyridyl groups.e After addition of tributylamine and subsequent treatment with trifluoroacetic acid in a stoichiometric amount with respect to the previously added amine.f At scan rates higher than 1 V s−1 this process gains reversibility (E1/2 = +1.20 V).g Four-electron transfer process. | |||||
1·H2+ | CH2Cl2 | +1.45bc | −0.40 | −0.82 | |
1+d | CH2Cl2 | +1.28bc | −0.67b | −0.82 | |
1·H2+e | CH2Cl2 | +1.51bc | −0.42 | −0.72 | |
1·H2+ | MeCN | +1.31cf | −0.42 | −0.80 | |
1+d | MeCN | +1.28cf | −0.86c | ||
1·H2+e | MeCN | +1.30cf | −0.44 | −0.78 | |
3·H24+ | MeCN | −0.43c | −0.79c | ||
32+d | MeCN | −0.82g | |||
3·H24+e | MeCN | −0.47c | −0.80c | ||
4 | CH2Cl2 | +1.48b | +1.28b | ||
4 | MeCN | +1.32b | +1.16b |
Under the experimental conditions used (6.0 × 10−4 mol L−1), the 1 ·H2+ species adopts a self-threaded conformation in CH2Cl2 , while in MeCN most of the molecules are involved in intermolecular complexes, as evidenced by the spectroscopic investigation at different 1·H2+ concentrations (see above). In both solvents the experimental cyclic voltammetries show two reversible one-electron reduction processes, and a chemically irreversible two-electron oxidation process which becomes reversible only at scan rates higher than 1 V s−1 in MeCN solution.
By comparison with model compound 3·H24+ (Fig. 3, Table 1), which is soluble only in MeCN, we can assign the two reduction processes of 1·H2+ to the two successive reductions of the bipyridinium unit. After addition of a stoichiometric amount of tributylamine, the reduction potential is shifted toward more negative potentials, as expected for the pyridyl(pyridinium) unit of the deprotonated form 1+ (Table 1). It should be noted that, in MeCN solution, after the addition of the amine, both 1+ and the model compound 32+ show only one peak, which corresponds to the transfer of two electrons. This behavior can be explained tentatively by an ECE (electrochemical–chemical–electrochemical) mechanism, as illustrated in eqn. (1) for 1+. The monoreduced pyridyl(pyridinium) unit of 1 is protonated by the tributylammonium cation, leading to a 1·H+ species with a standard potential less negative than that of 1+. Addition of trifluoroacetic acid restores the initial electrochemical pattern, confirming the reversibility of the deprotonation process and the resistance of the system to base/acid stimulation, as observed in the spectroscopic studies.
(1) |
The two-electron oxidation process of compound 1·H2+ is likely to involve both the 1,5-DON and 1,3-DOB units. Crown ether 4 (Fig. 3, Table 1) is a satisfactory model for the 1,5-DON, but not for the 1,3-DOB, unit of 1·H2+ since (i) 1,3-dimethoxybenzene is oxidized at more positive potentials than 1,4-dimethoxybenzene,26 and (ii) the 1,3-DOB unit of 1·H2+ bears a 4,4′-bipyridinium substituent. The results show that the oxidation of the 1,5-DON unit of 1 ·H2+ occurs at more positive potentials than in the case of compound 4. This observation is fully consistent with the engagement of the 1,5-DON unit in CT interactions with the 4,4′-bipyridinium unit, and is consistent with the spectroscopic results (see above).
In CH2Cl2 solution it might be expected (eqn. 2) that the one-electron oxidized form 1·H3+ undergoes dethreading because of electronic repulsions and the disruption of CT interactions. Oxidation of the 1,3-DOB unit should therefore take place in the dethreaded structure, but the lack of suitable model compounds does not allow us to discuss this possibility.
(2) |
Inspection of CPK space-filling molecular models show that compound 24+ can undergo self-complexation, as indicated in Fig. 9. In the solid state, the 1,5-DON unit is indeed sandwiched between the two bipyridinium units, a structure which is stabilized by π–π stacking interactions and by [C–H···O] hydrogen bonds.9a NMR Spectroscopic analysis indicated that such a self-complexed structure is maintained in CD3CN solution at 233 K, and that a high temperature (309 K) rotation can occur about the –CH2–C6H2R2–CH2– axis of the disubstituted p-xylyl group.9a The absorption spectrum of 24+ in MeCN solution is shown in Fig. 10, together with the sum of the spectra of its chromophoric component units, taken as 1,1′-dibenzyl-4,4′-bipyridinium, 1,4-dimethoxybenzene and 1,5-dimethoxynaphthalene. The rather intense tail in the 320–400 nm region (ε = 2500 L mol−1 cm−1 at 350 nm) can be assigned to a through-bond CT interaction between the 1,4-DOB and 4,4′-bipyridinium units, whereas the much weaker and broad absorption band with a maximum at 560 nm compares well with the CT band found for pseudorotaxanes comprised of a 1,5-DON unit threaded through a tetracationic macrocycle containing two 4,4′-bipyridinium units.5c,7a These results confirm that the stable conformation of compound 24+ is the self-complexed one (Fig. 9a).
Fig. 9 Cartoon representation of the two possible conformations of compound 24+. |
Fig. 10 Absorption spectrum of compound 24+ (dashed line), and sum of the spectra of its chromophoric units, 4,4′-bipyridinium, 1,4-DOB and 1,5-DON (full line) in MeCN at 298 K. |
In compound 24+ the fluorescence of the 1,5-DON unit is strongly quenched (>200 times), with a residual emission that, by evaluation of its lifetime, can be assigned to small amounts of 1,5-dimethoxynaphthalene-type impurities.
Compound | E/V s. SCEa | |||
---|---|---|---|---|
a Halfwave potential values (E1/2), unless otherwise noted.b Chemically irreversible process; Epa value at scan rate of 0.2 V s−1.c Two-electron transfer process.d At 228 K a splitting of this process is observed.e Data from ref. 12.f Data from ref. 13. | ||||
24+ | +1.62b | +1.50b | −0.40cd | −0.80c |
4 | +1.32b | +1.16b | ||
54+e | −0.29c | −0.71c | ||
64+f | +1.51bc | −0.35c | −0.80c |
Fig. 11 Scheme of the electrochemically controlled mechanical movements that can take place in compound 24+. |
In the anodic region compound 24+ shows two distinct one-electron chemically irreversible oxidation processes that have to involve the 1,5-DON and 1,4-DOB units. Although 4 is a good model for the 1,5-DON unit of 24+, it is not so good for the 1,4-DOB unit, which carries, in 24+, strong electron-acceptor substituents.28 The results show (Table 2) that oxidation of the 1,5-DON unit of 24+ occurs at much more positive potentials than in the case of compound 4. This observation is fully consistent with a self-complexed conformation (Fig. 9a), as suggested by the spectroscopic results (see above). The second oxidation process of 24+ can be assigned to its 1,4-DOB unit. The lack of good model compounds does not allow us to establish whether such an oxidation occurs in the original self-complexed conformation or in the decomplexed one. Clearly, in the one-electron oxidized form 25+, the presence of electrostatic repulsion and the disappearance of the CT interaction that stabilizes the self-complexed conformation of 24+ are expected to cause escape of the positively charged 1,5-DON unit from the cavity of the tetracationic macrocycle (Fig. 11b).
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