Cristin E.
Juda
,
Rex C.
Handford
,
Amymarie K.
Bartholomew
,
Tamara M.
Powers
,
Nina X.
Gu
,
Elisabeth
Meyer
,
Nikolaj
Roth
,
Yu-sheng
Chen
,
Shao-Liang
Zheng
and
Theodore A.
Betley
*
Department of Chemistry and Chemical Biology, Harvard University, Cambridge, MA 02139, USA. E-mail: betley@chemistry.harvard.edu
First published on 15th February 2024
Stepwise metalation of the hexadentate ligand tbsLH6 (tbsLH6 = 1,3,5-C6H9(NHC6H4-o-NHSiMe2tBu)3) affords bimetallic trinuclear clusters (tbsL)Fe2Zn(thf) and (tbsL)Fe2Zn(py). Reactivity studies were pursued to understand metal atom lability as the clusters undergo ligand substitution, redox chemistry, and group transfer processes. Chloride addition to (tbsL)Fe2Zn(thf) resulted in a mixture of species including both all-zinc and all-iron products. Addition of ArN3 (Ar = Ph, 3,5-(CF3)2C6H3) to (tbsL)Fe2Zn(py) yielded a mixture of two trinuclear products: (tbsL)Fe3(μ3-NAr) and (tbsL)Fe2Zn(μ3-NAr)(py). The two imido species were separated via crystallization, and outer sphere reduction of (tbsL)Fe2Zn(μ3-NAr)(py) resulted in the formation of a single product, [2,2,2-crypt(K)][(tbsL)Fe2Zn(μ3-NAr)]. These results provide insight into the relationship between heterometallic cluster structure and substitutional lability and could help inform both future catalyst design and our understanding of metal atom lability in bioinorganic systems.
We are particularly interested in investigating metal atom lability in synthetic heterometallic clusters given the prevalence of metalloenzyme heterometallic cofactors (e.g., nitrogenase cofactors,1–4,24–26 carbon monoxide dehydrogenase,27–30 OEC,5–9,31,32 and the Mn/Fe cofactor in ribonucleotide reductase,33–35 see Fig. 1) as well as their conformational lability in during reactivity (e.g., nitrogenase, OEC).24,26,29–32 Given these motivations we sought to use a mixed-metal system to uncover fundamental principles of how cluster binding geometry and reactivity relate to metal atom lability within synthetic analogues.
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Fig. 1 Example heterometallic cofactors in nature: (a) nitrogenase, (b) carbon monoxide dehydrogenase, (c) oxygen evolving complex, and (d) MnFe ribonucleotide reductase. |
Our lab has previously employed a hexadentate ligand, 1,3,5-C6H9-(NHC6H4-o-NHSitBuMe2)3 (tbsLH6), to yield both homo-21,36–38 and hetero-trinuclear39 clusters, including reactive, high spin (tbsL)Fe3(thf) (1) and (tbsL)Fe3(py) (2). Treatment of 1 with small molecule substrates results in multi-electron bond activation processes.36 Previous work by our lab has also demonstrated that reactive, high-spin clusters can undergo metal atom metathesis.40 Therefore, to test the metal atom lability of our clusters during reactions, we sought to explore reaction chemistry on a heterometallic trinuclear cluster. In this work, we describe the synthesis of [Fe2Zn] clusters and assess their substitutional integrity as they undergo substrate binding, oxidative group transfer, and outer sphere redox chemistry. In both substrate binding and group transfer chemistry, we observe redistribution of metals, whereas in the presence of a μ3-imido cap on the clusters, the cluster core maintains its integrity during redox processes. The results presented herein illustrate that for open-shell clusters, metal atom exchange can be facile even when starting with substitutionally homogeneous materials. This point is especially important given the formation of heterometallic enzymatic cofactors that do not necessarily feature electronically differentiated binding sites. Thus, formation of heterometallic species might form under mild conditions.
SC-XRD studies of 5 (Fig. 2a) and 6 (Fig. S37†) reveals C1-symmetric complexes containing a [Fe2Zn] core, isostructural to 1 and 2. The average M–M distances of 5 (dFe–Fe: 2.7354(9) Å, dFe–Zn: 3.051(1) Å) and 6 (dFe–Fe: 2.8141(7) Å, dFe–Zn: 2.9366(8) Å) are longer than the average M–M distances in the tri-iron cores of 1 (2.577(6) Å)11 and 2 (2.608(1) Å). Stabilization of the triiron core via direct exchange pathways results from short Fe–Fe contacts, thus incorporation of zinc, which does not participate in this exchange, increases the average M–M separation.37 We assigned the two metal sites with the shortest M–M contact as iron, leaving zinc at the three-coordinate site (Fig. 2a). X-ray fluorescence (XRF) spectroscopy was used to determine the bulk metal composition of the crystalline samples. Using a calibration curve to correct for the differential absorption power of the two metals, the Fe:
Zn molar ratios were measured as 2.2
:
1 for 5 and 2.1
:
1 for 6. These values are consistent with the expected 2
:
1 ratio.
Zero-field 57Fe Mössbauer spectroscopy (57Fe MB) analysis of 1 and 2 reveals three iron environments in each (δ, |ΔEQ| (mm s−1) (%) for 1:36–38 0.88, 1.29 (28%); 0.37, 1.99 (36%); 0.46, 1.52 (36%); for 2: 0.33, 1.84 (38%); 0.55, 1.76 (28%); 0.74, 1.39 (33%); Fig. S1†). However, only two quadrupole doublets are observed for 5 and 6, indicating site-isolated insertion of zinc into the trinuclear core (δ, |ΔEQ| (mm s−1) for 5: 0.60, 1.83 (50%); 0.84, 1.55 (50%); for 6: 0.61, 1.68 (50%); 0.79, 1.63 (50%); Fig. 2a and S4†). Compared to 1 and 2, 5 and 6 lack a quadrupole doublet with an isomer shift near 0.3 mm s−1, corresponding to the three-coordinate site in the core.
The electronic structure of 5 was further interrogated by study of its magnetic susceptibility via SQUID magnetometry. A plot of XMT vs T indicates that 5 possesses a low-spin ground state (XMT (2.0 K) = 0.73 cm3 K mol−1). Beyond 100 K, the susceptibility increases monotonically with temperature, reaching a value of 3.99 cm3 K mol−1 at 300 K (Fig. 3a). Low-temperature magnetization studies of 5 reveal a saturation magnetization value of 0.58 NAμB, suggestive of a diamagnetic ground state for 5 with a small population of paramagnetic states remaining. The electronic structure of 5 stands in contrast to the structurally analogous, maximally high-spin S = 6 triferrous cluster (tbsL)Fe3(thf) (1).21 The susceptibility of 1 increases rapidly from 1.8 to 20 K from an initial value of 13.75 cm3 K mol−1, reaching a maximum of 19.33 cm3 K mol−1 at 150 K, and diminishing moderately to 17.80 cm3 K mol−1 at 300 K (Fig. 3a). A low-temperature magnetization study of triiron 1 reveals a saturation magnetization value of 8.32 NAμB, which is below the value anticipated for a maximally high-spin S = 6 system, in line with the presence of zero-field splitting (Fig. 3b). The susceptibility and magnetization data of 1 were best fit to a spin-Hamiltonian describing three coupled spins in an equilateral arrangement, providing J = 40(1) cm−1, D = 20.0(9) cm−1, |E/D| = 0.082(7) cm−1, and g = 1.92(1) (see ESI†). These data reveal that in 5, magnetic coupling of the two iron centers is dominated by antiferromagnetic superexchange through the dianilido bridge, and further suggests that the high-spin ground-state of isostructural (tbsL)Fe3(thf) (1) is strongly influenced by the incorporation of a third ferrous ion.
While the bulk metal ratio of (tbsL)Fe2Zn(thf) (5) was conserved upon chloride ligation, the 1H NMR spectrum of redissolved crystalline material (Fig. S20†) shows the all-iron and all-zinc clusters [NBu4][(tbsL)Fe3(μ3-Cl)] (7) and [NBu4][(tbsL)Zn3(μ3-Cl)] (8), alongside mixed-metal cluster 9. These data indicate that chloride anion substitution of THF in 5 results in metal atom redistribution. Indeed, the substitution of a labile ligand for chloride seems to be a determining factor in facilitating metal atom redistribution. Notably, such redistribution reactivity is hindered in an equimolar mixture of the μ3-halide capped complexes 7 and 8 (Scheme 3). In THF solution, 7 and 8 showed no evidence of metal atom redistribution after 24 h at room temperature, with only trace amounts of mixed-metal products forming after heating to 80 °C, according to 1H NMR spectroscopy (Fig. S21†). In contrast, 1H NMR analysis of a solution containing 5 and tri-ferrous 7 revealed complete consumption of 5 to generate 9, with some 7 persisting in solution (Scheme 3 and Fig. S22†). In contrast, reaction of 5 with all-zinc 8 produced only trace quantities of 9 at room temperature, with only modestly greater conversion upon heating to 60 °C (Fig. S23†). The qualitatively slower redistribution reactivity of 5 with 8 (compared to 7) is likely a manifestation of the greater Lewis acidity of the [Zn3] core relative to the [Fe3] core, which results in stronger binding of the μ3-chloride cap.
The structure of 11 was confirmed via a SC-XRD study. As in 10, the imido moiety is bound μ3 to the face of the trinuclear core, and tbsL is arranged in a C3-symmetric orientation. An elongation of the average M–M contact in 11 (2.701(1) Å vs. 2.530(1) Å in 10), supports the presence of zinc. Treatment of the py-bound species 6 with PhN3 also resulted in a mixture of a new product and 10 by 1H NMR. Unlike the reaction of 5 with PhN3, crystallization from hexane at −33 °C cleanly separates the new paramagnetic product from 10.
SC-XRD analysis of this new product reveals a C1-symmetric cluster, (tbsL)Fe2Zn(μ3-NPh)(py) (12) (Fig. S42†). In contrast to the reaction of 2 with PhN3, which produces unsolvated 10, pyridine remains bound to one metal center in 12. We assigned the py-bound site as the zinc site as it also features the longest M–M separations (2.7599(6), 3.2059(7) Å). The remaining two atoms are assigned as the iron positions, supported by the short M–M contact between these sites (2.4880(6) Å). The Fe–Fe contact in this species is shorter than all three Fe–Fe contacts in 10. This shortened Fe–Fe distance is suggestive of an increased M–M interaction, consistent with localization of two-electron oxidation across two iron sites. The 57Fe MB spectrum of 12 exhibits two quadrupole doublets due to the differences in coordination environment at the two iron centers (δ, |ΔEQ| (mm s−1): 0.35, 2.76 (49%); 0.33, 1.80 (51%); Fig. S8†). However, the similar isomer shift of the two signals confirms that both iron centers are in the 3+ oxidation state. The XRF spectrum of crystalline 12 gave an Fe:
Zn ratio of 2.1
:
1, consistent with a compositionally homogenous [Fe2Zn] cluster (Fig. S17†).
To quantify metal atom redistribution, 6 was treated with 3,5-bistrifluoromethyl-azidobenzene (3,5-(CF3)2C6H3N3), which allowed for integration of the product ratio via19F NMR spectroscopy. Two resonances were observed in the 19F NMR spectrum of the reaction mixture in a 7.8:
1 ratio, where the less intense peak at −69.4 ppm was identified by independent synthesis as the triiron imido (tbsL)Fe3(μ3-N(3,5-(CF3)2C6H3)) (13), confirming formation of (tbsL)Fe2Zn(μ3-N(3,5-(CF3)2C6H3))(py) (14) as the major product. Akin to 12, cluster 14 can be selectively crystallized and SC-XRD analysis of 14 revealed a structure directly analogous to 12 (Fig. 2c). The XRF spectrum of crystalline 14 yielded an Fe
:
Zn ratio of 2.1
:
1.
Crystals of the product were formed by diffusion of hexanes into a concentrated THF solution at −33 °C. SC-XRD analysis confirmed that the imido ligand remains μ3-bound, while pyridine has been expelled to form the mixed-metal imido cluster [2,2,2-crypt(K)][(tbsL)Fe2Zn(μ3-NArF)] (16) (Fig. 2d). The three metal sites span a modest range with respect to M–Nimido distances from the two molecules in the asymmetric unit (2.010(2)–2.101(3) Å) and M–M separation (2.6660(7)–2.7843(6) Å). Despite its geometric symmetry, 16 exhibits two quadrupole doublets in its 57Fe MB spectrum. While one doublet has a similar isomer shift to that of the two quadrupole doublets in the starting material (0.35 mm s−1), the other increases to 0.59 mm s−1 (Fig. 2d), consistent with site-isolated reduction.42 As it is impossible to discern the metal identity of the three sites by traditional X-ray diffraction, we are currently investigating 16 using resonant X-ray and neutron diffraction to evaluate the metal occupancy at each site.
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Scheme 4 Metal-atom metathesis from mixed valent cluster (PhL)Fe3Cl(thf) see ref. 43. |
Azide binding likely facilitates metal atom extrusion akin to the chloride addition, particularly in instances where the azide ligand is bound in a terminal, μ1-fashion.44 While the mixed-metal imido clusters 12 and 14 could be trapped and selectively crystallized, monitoring of the reaction between 6 and ArN3 indicated metal atom redistribution, as evidenced by the formation of the triiron imido, (tbsL)Fe3(μ3-NAr). Again, exchange of L′ for NAr, followed by (tbsL) reorganization about the trinuclear core, can expose the azide-bound metal to facilitate exchange. For example, organic azide binding in the structurally analogous [Cr3] cluster (tbsL)Cr3(thf) produces different end products (i.e., bridging nitride vs. terminal imido, Scheme 5) depending on how the reacting azide binds to the all-chromous cluster.44
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Scheme 5 Solvent directed change in azide breakdown. See ref. 44. |
We propose that open-faced clusters (e.g., non-symmetrical binding of the templating ligand about the trinuclear core) are necessary to facilitate metal-atom exchange. This is bolstered by the observation that there appears to be little accumulation of free ligand following the metal-atom redistribution. However, we cannot rule out that small amounts of in situ generated MX2 species are aiding in the metal atom redistribution reactions; notably, added MX2 salts have been shown to catalyze metal-atom exchange in related clusters.43 Indeed, treatment of 5 with FeCl2 (one equiv.) in THF solution resulted in rapid metal redistribution to form 9 at room temperature (Fig. S24†), although additional unidentified paramagnetic species were also generated, according to 1H NMR spectroscopy. Surprisingly, no redistribution was observed from a mixture of 5 with ZnCl2 (one equiv.) in THF solution, although a diminution of overall resonance intensity in the 1H NMR spectrum (Fig. S25†), as well as a color change from brown to purple, suggested that a transformation had occurred.
While metal-atom shuffling was observed upon both neutral substrate-binding and oxidative group transfer chemistry, the integrity of our mixed-metal clusters was maintained upon outer sphere electron transfer when stabilized by an imido capping group. This stabilization is consistent with previous work in cluster chemistry, which has employed bridging ligands to prevent cluster degradation during reactivity.45–47 The results of this inquiry allow us to demonstrate the dynamic nature of cluster reaction sites. Moreover, knowledge of the factors which confer stability to these clusters can provide valuable information to be used in future catalyst design. Finally, these results illustrate the dynamic nature of bimetallic reaction site substitutions, which may be relevant not only for synthetic cofactor analogues, but also for biological cofactors themselves.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 1993457–1993469. For ESI and crystallographic data in CIF or other electronic format see DOI: https://doi.org/10.1039/d3sc03606e |
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