Dynamic Complex-to-Complex Transformations of Heterobimetallic Systems Influence the Cage Structure or Spin State of Iron(II) Ions.

Two new heterobimetallic cages, a trigonal-bipyramidal and a cubic one, were assembled from the same mononuclear metalloligand by adopting the molecular library approach, using iron(II) and palladium(II) building blocks. The ligand system was designed to readily assemble through subcomponent self-assembly. It allowed the introduction of steric strain at the iron(II) centres, which stabilizes its paramagnetic high-spin state. This steric strain was utilized to drive dynamic complex-to-complex transformations with both the metalloligand and heterobimetallic cages. Addition of sterically less crowded subcomponents as a chemical stimulus transformed all complexes to their previously reported low-spin analogues. The metalloligand and bipyramid incorporated the new building block more readily than the cubic cage, probably because the geometric structure of the sterically crowded metalloligand favours the cube formation. Furthermore it was possible to provoke structural transformations upon addition of more favourable chelating ligands, converting the cubic structures into bipyramidal ones.

Metallosupn>ramolecular chemistry1 has produced many beautiful structures with defined shapes2 and fascinating functionality.3 Within metallosupramolecular chemistry, a powerful tool is the subcomponent self‐assembly approach, in which aggregates emerge from the assembly of two ligand subunits that form feasible ligands and their complexes in situ. These are formed via the reversible formation of covalent bonds.4 This approach was used to prepare numerous structures adopting various properties and features,5 for example, host–guest complexes [6] and switchable systems.6c, 7 The tuning of complex properties is often facilitated by varying one distinct ligand subunit and exchanging one building block.6b, 8 In combination with the reversible character of the covalent bonds, these properties can also allow for building block exchanges in situ, resulting in complex‐to‐complex transformations.7a, 9 Besides subcomponent exchanges, also ligand exchanges,10 solvent dependencies,11 and light irradiation12 were successfully used to perform complex‐to‐complex transformations.

Aside from indisputably beautiful homometallic structures, the subcompn>onent self‐assembly apn>proach also proved useful for the formation of heterobimetallic cages within the context of the complex‐as‐a‐ligand strategy.13 Thus, it is possible to transfer all advantages of the subcomponent self‐assembly approach to systems consisting of more than one type of metal cation. However, to date only a few examples of heterobimetallic complexes have been reported that were built up from subcomponents.13d, 13e, 14

Previously, Drago et al. introduced a ligand system that can be prepared from the commercially available building blocks tris(2‐aminoethyl)amine (TREN), 2‐formylpyridine, 2‐formyl‐6‐methyln>an class="Chemical">pyridine, and iron(II) salts.15 2‐Formyl‐6‐methylpyridine‐containing complexes show a stabilization of the high‐spin state of iron(II) cations at room temperature due to steric strain between the methyl groups and nearby pyridine rings, as well as spin‐crossover behaviour in the solid state.15, 16 These aldehydes were also used to develop 3D architectures with different shapes and sizes that show complex‐to‐complex transformations upon replacement of 2‐formyl‐6‐methylpyridine with less bulky 2‐formylpyridine. These transformations resulted in a change of the spin state of iron(II) cations from high spin to low spin, due to shortening of the Fe−N bonds.9b, 17 The decrease of steric strain might be responsible for the preferential incorporation of 2‐formylpyridine over 2‐formyl‐6‐methylpyridine.9b, 17

In this work we investigated the dynamic behaviour of heterobimetallic structures that assemble through subcompn>onent self‐assembly. These compn>lexes contain sterically strained n>an class="Chemical">iron(II) centres in the paramagnetic high‐spin state. We adopted previously reported subcomponent exchanges and expanded these principles to heterometallic systems. Chemical stimuli transferred the heterobimetallic paramagnetic complexes to their diamagnetic analogues upon reduction of steric strain. In addition, we could perform ligand‐exchange reactions, resulting in the structural transformation of cubic to bipyramidal cages.

Ditopic building block 1 was selected to achieve the formation of C 3‐symmetric iron(II) tris(pyridylimine) moieties18 as well as C 2‐ and C 4‐symmetric n>an class="Chemical">palladium(II) pyridine moieties. Reaction of 3 equivalents of aldehyde 1 with 1 equivalent of TREN 2 and 1 equivalent of iron(II) tetrafluoroborate hexahydrate in acetonitrile yielded the mononuclear complex ML‐1(BF4)2 as a bright red solid (Scheme 1). This mononuclear complex was characterised by 1H NMR and UV/Vis spectroscopy, ESI‐MS spectrometry, vibrating sample magnetometry, and single‐crystal X‐ray diffraction (see the Supporting Information). Mixing 1 equivalent of ML‐1(BF4)2 with 1.5 equivalents of 1,3‐bis(diphenylphosphino)propane palladium(II) triflate ([(dppp)Pd(OTf)2]) or 0.75 equivalents of tetrakis(acetonitrile) palladium(II) tetrafluoroborate ([Pd(CH3CN)4](BF4)2) in acetonitrile resulted in the formation of heterometallic pentanuclear bipyramidal assembly BP‐1(OTf)6(BF4)4 or the tetradecanuclear cubic assembly CU‐1(BF4)28, respectively, each as a bright red microcrystalline solid in high yields (Scheme 1).

Scheme 1

Stepwise self‐assembly of BP‐1(OTf)6(BF4)4 and CU‐1(BF4)28 via formation of ML‐1(BF4)2 from 1 and 2.

Stepwise self‐assembly of BP‐1(OTf)6(BF4)4 and n>an class="Chemical">CU‐1(BF4)28 via formation of ML‐1(BF4)2 from 1 and 2.

The identity and purity of bipyramid BP‐1(OTf)6(BF4)4 were proven by n>an class="Chemical">1H NMR and UV/Vis spectroscopy and ESI‐MS (see the Supporting Information). When vibrating sample magnetometry and the Evans’ method19 were employed, a magnetic susceptibility of Χ m T=6.0 cm3 K mol−1 was revealed, which is in very good agreement with the expected value for two uncoupled iron(II) cations in the high‐spin state (6.001 cm3 K mol−1).20 Slow diffusion of diethyl ether into a concentrated solution of BP‐1(OTf)6(BF4)4 in acetonitrile gave X‐ray diffraction quality single crystals that could be used to determine its crystal structure (Figure 1). The mixed anionic cage BP‐1(OTf)6(BF4)4 crystallises in the monoclinic space group C2/c, with both homochiral enantiomers [(Δ,Δ) and (Λ,Λ)] present in the unit cell as a racemic mixture and is best described as a trigonal bipyramid or helicate21 (for more details see the Supporting Information).

Figure 1

Structure of bipyramidal complex BP‐1(OTf)6(BF4)4 as determined by single‐crystal X‐ray diffraction. Hydrogen atoms, counter ions and solvent molecules are omitted for clarity; colour code: grey C, blue N, yellow‐orange P, dark orange Fe, turquoise Pd.

Structure of bipyramidal complex BP‐1(OTf)6(BF4)4 as determined by single‐crystal X‐ray diffraction. n>an class="Chemical">Hydrogen atoms, counter ions and solvent molecules are omitted for clarity; colour code: grey C, blue N, yellow‐orange P, dark orange Fe, turquoise Pd.

The iron cations are coordinated in an octahedral ligand spn>here with an average n>an class="Chemical">Fe−N bond length of 2.179 Å, consistent with a paramagnetic high‐spin iron(II) complex.22 The palladium centres form the equatorial plane of the complex and are settled in a square‐planar ligand sphere, each coordinated by a bidentate dppp ligand and two 4‐pyridyl moieties.

The identity of the heterobimetallic cube CU‐1(BF4)28 could also be proven by 1H NMR and UV/Vis spectroscopy and ESI‐MS (see the Supporting Information). An Evans’ experiment revealed a magnetic susceptibility of X m T=24.1 cm3 K mol−1, proving its fully paramagnetic character.20 Interestingly, the self‐assembly of CU‐1(BF4)28 was completed after only 16 hours at 50 °C, whereas the self‐assembly of a previously reported diamagnetic analogue13e of this heterobimetallic cube required 120 hours under the same conditions. We attribute this tremendously shorter reaction time of CU‐1(BF4)28 to the larger opening angle of ML‐1(BF4)2, compared to the metalloligand without the additional methyl groups on the pyridine binding to the iron(II) ion. Due to the steric strain around the iron centre, the opening angle becomes larger, and therefore, should be better preorganized to form the heterobimetallic cube.

Very slow evaporation of solvent from an acetonitrile solution of n>an class="Chemical">CU‐1(BF4)28 over 3 months yielded single crystals, which diffracted up to 1.2 Å using synchrotron radiation23 and allowed for unambiguous structure determination (Figure 2).

Figure 2

Structure of cube CU‐1 as determined by single‐crystal X‐ray diffraction using synchrotron radiation. Eight tetrafluoroborate anions occupy the inner void. Hydrogen atoms, solvent molecules, and counter ions outside the cavity are omitted for clarity; colour code: grey C, blue N, light green F, brown‐beig B, dark orange Fe, turquoise Pd.

Structure of cube n>an class="Chemical">CU‐1 as determined by single‐crystal X‐ray diffraction using synchrotron radiation. Eight tetrafluoroborate anions occupy the inner void. Hydrogen atoms, solvent molecules, and counter ions outside the cavity are omitted for clarity; colour code: grey C, blue N, light green F, brown‐beig B, dark orange Fe, turquoise Pd.

CU‐1(n>an class="Chemical">BF4)28 crystallises in the cubic space group Fm− c with both homochiral enantiomers [all (Δ) and all (Λ)] present in the unit cell as a racemic mixture. Only one‐third of one ligand and one iron ion is found in the asymmetric unit due to the threefold symmetry axis. All three Fe−N bonds are crystallographically equivalent and show a bond length of 2.105(11) Å, which is consistent with a high‐spin iron(II) complex. The tetravalent palladium ions with their four coordinated pyridine moieties are located on the fourfold symmetry axes of the cubic cage. Eight tetrafluoroborate anions occupy the void of the cage, adapting the cubic arrangement themselves.

The steric strain in ML‐1, BP‐1, and CU‐1 results in an elongation of the n>an class="Chemical">Fe−N bond lengths and the stabilization of the paramagnetic high‐spin state.9b, 15, 17 Still the situation is energetically unfavourable, and hence, can be exploited in thermodynamically driven complex‐to‐complex transformations during which the steric strain is reduced. The transformation reactions were performed by the addition of a twofold excess of sterically less crowded 2‐formyl‐5‐(4′‐pyridyl)pyridine 3 (per exchangeable methyl‐substituted aldehyde component) to the complex solutions and were monitored by 1H NMR spectroscopy. In such a scenario a quantitative incorporation of 3 would lead to a 50:50 or 1:1 ratio of both free aldehydes 1 and 3. Please note that we had to analyse the signals of the individual aldehyde subcomponents as probes here as integration of 1H NMR signals of paramagnetic species is generally not possible, when mixed species with different magnetic properties are present.

Following this approach, addition of 6 equivalents of 3 to a solution of ML‐1(BF4)2 released free 3 equivalents of subcompn>onent 1 when 3 was incorpn>orated almost quantitatively into the compn>lex, resulting in the formation of previously reported diamagnetic metalloligand ML‐2(BF4)2 in high yield (Scheme 2). Progress of this reaction was indicated by a change in the colour of the solution from bright red to dark purple. After 16 hours at 40 °C the mixture reached equilibrium with free subcomponents 3 and 1 in a 56:44 ratio and a new set of signals in the 1H NMR spectrum referring to ML‐2(BF4)2 (see the Supporting Information).

Scheme 2

Sterically driven complex‐to‐complex transformations. Red atoms mark iron(II) in the high‐spin state, purple atoms mark iron(II) in the low‐spin state.

Sterically driven complex‐to‐complex transformations. Red atoms mark iron(II) in the high‐spn>in state, purpn>le atoms mark n>an class="Chemical">iron(II) in the low‐spin state.

The same chemical stimulus can be used to transfer paramagnetic BP‐1(OTf)6(n>an class="Chemical">BF4)4 quantitatively into the corresponding diamagnetic cage BP‐2(OTf)6(BF4)4. After 16 hours at 40 °C the equilibrium ratio of 3 and 1 was determined to be 1:1 and 1H NMR signals arose that can be assigned to BP‐2(OTf)6(BF4)4 (see the Supporting Information). Also the formation of BP‐2(OTf)6(BF4)4 could be shown by UV/Vis spectroscopy (see the Supporting Information). This transformation impressively demonstrates the strong driving force of this subcomponent exchange and the highly dynamic behaviour of this heterobimetallic system. In the course of this exchange reaction, one covalent imine bond, two coordinative Fe−N bonds, and one coordinative Pd−N bond have to be broken, the new building block has to align and to reform all formerly cleaved bonds again for each exchanged subcomponent.

Similar treatment of cubic cage n>an class="Chemical">CU‐1(BF4)28 with a greater excess of 100 equivalents of 3 resulted in the transformation to the analogous diamagnetic cube CU‐2(BF4)28. Unlike with ML‐1(BF4)2 and BP‐1(OTf)6(BF4)4, however, the subcomponent exchange required considerably more time. After three days at 65 °C an equilibrium ratio between 1 and 3 of 30:70 was determined, which is close to the expected 24:76 ratio. However, the use of only 48 equivalents of 3 did not lead to a complete transformation (see the Supporting Information). Therefore, these experiments show that incorporation of 3 into the cubic assembly is slightly more favoured than incorporation of 1, but less pronounced than in the case of the bipyramidal assemblies.

Hence, in case of the cubic cage the sterically stressed compn>lex probably is not as disfavoured as for ML‐1(n>an class="Chemical">BF4)2 and BP‐1(OTf)6(BF4)4. The larger opening angle of ML‐1(BF4)2 caused by the additional methyl groups seems to be a better preorganization for the assembly of cubic structures than the smaller opening angle in ML‐2(BF4)2. This assumption is corroborated by the much faster formation of CU‐1(BF4)28 compared to that of CU‐2(BF4)28, although it is difficult to dissect whether this is due to the kinetics or the thermodynamics of the assembly process.

Besides sterically driven subcomponent‐exchange reactions that influence the spin state of iron(II) cations, the system also allows for structural conversions upn>on chemical stimulus, maintaining the initial spn>in state of the compn>lexes (see the Supn>porting Information). The addition of n>an class="Chemical">dppp as a chelating ligand to cubic cages CU‐1 and CU‐2 leads to complex‐to‐complex transformations, yielding the bipyramidal complexes BP‐1 and BP‐2 and excess metalloligands ML‐1 and ML‐2, respectively (Scheme 3, Supporting Information). In these reactions two 4‐pyridyl donors at palladium(II) cations are replaced by one bidentate dppp ligand, leading to major structural changes. Since the contingent of iron(II) cations in the cubic assemblies is greater than in the bipyramidal cages, excess metalloligand is produced as a side product in these transformations. Addition of 6 equivalents of dppp transforms one cubic cage into two bipyramidal assemblies and four free metalloligands, increasing the overall entropy of the system, which might be an additional driving force for this reaction besides the enthalpically strongly preferred coordination of the dppp ligand to palladium(II) cations to facilitate these conversions.24

Scheme 3

Structural transformations of cubic cages into bipyramidal complexes, producing the metalloligands as side products.

Structural transformations of pan class="Chemical">cubic cages into bipn>yramidal compn>lexes, producing the pan class="Chemical">metalloligands as side products.

In conclusion, we presented the stepwise assembly of two heterobimetallic cages BP‐1 and n>an class="Chemical">CU‐1 from the same C 3‐symmetric metalloligand ML‐1 adopting the well‐implemented molecular library approach. Compared to previously reported diamagnetic complexes ML‐2, BP‐2, and CU‐2 13e the simple addition of a methyl group in 6‐position of the pyridyl ring leads to a substantial amount of steric strain and changes the spin state of the iron(II) cations from diamagnetic low spin to paramagnetic high spin. This impressively shows how rather small changes of the ligand system can cause tremendous changes of the complex properties.

Paramagnetic complexes ML‐1 and BP‐1 showed a very high tendency to undergo subcomponent‐exchange reactions, resulting in the first reported complex‐to‐complex transformations of heterobimetallic compn>lexes to heterobimetallic complexes in which metal‐bridging components are exchanged. In this case, 2‐formyl‐6‐methyl‐5‐(4′‐pyridyl)‐pyridine 1 could be replaced by sterically less crowded 2‐formyl‐5‐(4′‐pyridyl)pyridine 3, transforming the high‐spin complexes into their low‐spin analogues.13e The cubic cage CU‐1, however, was found to exchange 1 much less readily, probably because the opening angle of the sterically crowded metalloligand makes it kinetically and thermodynamically favourable to assemble the cubic structure.

Addition of bidentate dppp to cubic assemblies CU‐1 and CU‐2 led to a ligand‐exchange reaction, in which two 4‐pyridyl donors around palladium(II) cations were replaced by the chelating ligand. These exchanges resulted in complex‐to‐complex transformations to the bipyramidal cages BP‐1 and BP‐2, respectively, maintaining the spin state of iron(II). Since the iron(II) to palladium(II) ratio decreases on going from the cubic to the bipyramidal cages, the corresponding free metalloligands ML‐1 and ML‐2 are formed as side products in these transformations. The presented complex‐to‐complex transformations beautifully show the highly dynamic behaviour of the heterobimetallic systems, allowing the change of magnetic or structural properties upon certain chemical stimuli.

Conflict of interest

The authors declare no conflict of interest.

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