Anders H.
Pedersen
a,
Miguel
Julve
b,
José
Martínez-Lillo
*b,
Joan
Cano
*b and
Euan K.
Brechin
*a
aEaStCHEM School of Chemistry, The University of Edinburgh, David Brewster Road, EH9 3FJ Edinburgh, UK. E-mail: E.Brechin@ed.ac.uk
bDepartament de Química Inorgànica/Instituto de Ciencia Molecular (ICMol), Universitat de València, C/Catedrático José Beltrán 2, Paterna, València, Spain. E-mail: joan.cano@uv.es; F.Jose.Martinez@uv.es
First published on 24th July 2017
Six novel one-dimensional chloro-bridged ReIVCuII complexes of formula {[Cu(L)4][ReCl6]}n, where L = imidazole (Imi, 1), 1-methylimidazole (Meim, 2), 1-vinylimidazole (Vim, 3), 1-butylimidazole (Buim, 4), 1-vinyl-1,2,4-triazole (Vtri, 5) and N,N′-dimethylformamide (DMF, 6) are characterised structurally, magnetically and theoretically. The structures exhibit significant differences in Cu–Cl bond lengths and Re–Cl–Cu bridging angles, resulting in large differences in the nature and magnitude of magnetic exchange interactions between the ReIV and CuII ions. Theoretical calculations reveal the coupling to be primarily ferromagnetic, increasing in magnitude as the bridging angle becomes smaller and the bond lengths shorten.
In this context, the most studied transition metal molecule-based magnets are polynuclear complexes based on paramagnetic 3d ions.2e In comparison, systems containing the heavier 4d and 5d ions have been much less explored, despite these metal ions being characterised by more radially extended magnetic orbitals (5d > 4d ≫ 3d) which results in larger spin delocalisation onto coordinated atoms/ligands creating stronger magnetic exchange between paramagnetic metal ions.3–5 The extremely large spin–orbit coupling constants (λ) of 4d and 5d ions is a direct cause of their unusually large zero-field splitting (zfs) values manifested in the axial (D) and rhombic (E) components, and highly anisotropic g-factors.4 Zero-field splitting plays an important role in the energy barrier for reversal of the magnetisation in these systems, and for this reason the 5d3 ReIV ion is of great interest due to its large magnetic anisotropy,5 which arises from second order spin–orbit coupling caused by a spin–orbit coupling constant for the free ion of λ ≈ 1000 cm−1.6 Apart from investigations into the magnetic properties of its salts (e.g. the effect of cation size on intermolecular interactions and Tc), the role of the [ReCl6]2− anion has been largely limited to that of synthetic precursor.6–19 Indeed, a common strategy for the creation of new ReIV complexes is the functionalisation of the [ReCl6]2− anion through halide exchange with ligands such as heterocyclic amines, pseudo halides such as cyanide, or chelates such as the oxalate anion.6,10–13 These species have subsequently been employed as metalloligands for the creation of larger oligomers.14–17 More recently, several 1D chains based on the ReIV ion have been reported. For example, the [trans-ReCl4(CN)2]2− anion was used to construct the Single-Chain Magnet (SCM) {[Fe(DMF)4][trans-ReCl4(CN)2]}n which displays a coercive field of 1 T at T = 1.8 K,9 the [ReF6]2− anion was used for the first time in 2014 as a metalloligand for the synthesis of the 1D complex {[Ni(Vim)4][ReF6]}n which exhibits strong ferromagnetic exchange between neighbouring metal ions,20 while the {[Cu(pyim)2][ReCl4(ox)]}n chain (pyim = 2-(2′-pyridyl)imidazole and ox = oxalate) exhibits ferrimagnetic behaviour due to the presence of two different magnetic exchange interaction pathways (O, Cl) between the ReIV and CuII ions.21 The possibility of using the [ReCl6]2− unit as a linker for neutral chains was introduced recently with the study of the species {[Cu(pyim)(Imi)2][ReCl6]}n (Imi = imidazole) which revealed antiferromagnetic exchange interactions and metamagnetic behaviour.22
This latter discovery has prompted us to search for more 1D networks based on the [ReCl6]2− anion, and herein we present six new chains which are characterised structurally, magnetically and theoretically. These chains are of general formula {[Cu(L)4][ReCl6]}n, where L = imidazole (Imi, 1), 1-methylimidazole (Meim, 2), 1-vinylimidazole (Vim, 3), 1-butylimidazole (Buim, 4), 1-vinyl-1,2,4-triazole (Vtri, 5) and N,N′-dimethylformamide (DMF, 6) (Scheme 1). The structures exhibit significant differences in Cu–Cl bond lengths and Re–Cl–Cu bridging angles, originating from the differences in the identity of the ligands (L) terminally bonded to the CuII ion. Combined with a theoretical examination of the magneto-structural relationship, a clear design principle for the construction of ferro- or antiferromagnetically coupled ReIV–CuII chains emerges.
Scheme 1 The ligands (L) employed: (a) imidazole, (b) 1-methylimidazole, (c) 1-vinylimidazole, (d) 1-butylimidazole, (e) 1-vinyl-1,2,4-triazole, (f) dimethylformamide. |
The chains crystallise in the triclinic space group P (1, 2 and 6), monoclinic space groups C2/c (3) and P21/c (5), and the orthorhombic space group Pccn (4) (Tables S1 and S2†). The asymmetric unit (ASU) of 1 contains two non-equivalent half molecules of the [Cu(Imi)4]2+ cation, one [ReCl6]2− anion and two isopropanol molecules (Fig. S1†). In 2, the ASU contains 1.5 molecules of the [Cu(Meim)4][ReCl6] motif, giving rise to two non-equivalent chains whose structural parameters deviate slightly (Fig. S2†). The ASUs of 3–6 contain half a cation and half an anion due to inversion centres located on the ReIV and CuII metal ions (Fig. S3–6†). One solvent acetonitrile molecule at 50% occupancy is also part of the ASU of 6.
In the crystal lattice of 1, the chains are oriented in a parallel fashion, and pack in layers in the crystallographic bc plane through C(H)⋯π interactions of ∼3.5 Å (C-atom to imidazole centroid) and N(H)⋯Cl interactions of ∼3.2 Å (Fig. S7†). The co-crystallised isopropanol molecules pack through O(H)⋯O and N(H)⋯O hydrogen bonds in the crystallographic bc plane between layers of chains. In the extended structure of 2, the chains travel parallel to the crystallographic b axis and pack via a range of C(H)⋯π, Cl⋯π and Cl⋯Cl interactions. Adjacent [Cu(Meim)4]2+ units pack through C(H)⋯π interactions of ∼3.6–3.8 Å, with the [ReCl6]2− anions packing through Cl⋯π (intra- and inter-chain) and Cl⋯Cl (inter-chain) interactions (Fig. S8†). The [ReCl6]2− anions have short Cl⋯π interactions of ∼3.6–3.8 Å to the cations and inter-chain Cl⋯Cl interactions of ∼3.9 Å between anions (Fig. S8b†).
The chains in 3 are ordered in 2D networks in the crystallographic ab plane, with each 2D network being pseudo-perpendicular to adjacent layers at an inter-chain angle of 81.45° (Fig. S9†). The chains pack through an extended network of Cl⋯π and C(H)⋯π interactions, with the shortest intra- and inter-chain Cl⋯π/C(H)⋯π interactions being approximately 3.4 Å and 3.6–3.9 Å, respectively (Fig. S10†). In 4, the chains describe a ‘grid’ like pattern down the crystallographic c axis (Fig. S11†). Each chain is well isolated from its nearest neighbours on account of the bulkiness of the butyl group of the imidazole ligands, which causes the inter-chain metal⋯metal distances to be >9 Å.
In the crystal lattice of 5, the chains propagate down the crystallographic a axis and pack through a myriad of intra- and inter-chain C(H)⋯N and Cl⋯π interactions. In each neutral chain, two short Cl⋯π interactions of ∼3.4 and ∼3.7 Å are present (Fig. S12a†) with the chains packing through short inter-chain C(H)⋯N interactions between triazole groups, and Cl⋯π interactions from the anions to the vinyl groups (Fig. S12b†). These C(H)⋯N interactions are of the order 3.2 Å, with inter-chain Cl⋯π distances of approximately 3.6 Å. The molecular chains of 6 are oriented in a parallel manner down the crystallographic c axis, with the acetonitrile molecules of crystallisation in the voids between the chains (Fig. S13†). The [ReCl6]2− unit interacts with the DMF ligands and acetonitrile solvate molecules through C(H)⋯Cl contacts, with C⋯Cl distances in the range of 3.5 to 3.8 Å (Fig. S14a†). C(H)⋯N interactions link the DMF ligands with the acetonitrile molecules, with C⋯N distances of approximately 3.3 and 3.6 Å (Fig. S14b†).
Quantitative analysis of the magnetic behaviour of ReIV compounds is non-trivial, since one must consider both intra- and inter-molecular exchange interactions caused by the strong delocalisation of spin density from the ReIV ion to the coordinated ligands (the latter can be as strong as the former), different g-values for the constituent metal ions (gRe and gCu), and zero-field splitting effects (DRe).5 In addition we note that some of these parameters are correlated: for example, erroneously large antiferromagnetic intra- or inter-molecular exchange can be deduced at the expense of underestimating zfs, whilst large ferromagnetic exchange is linked to an overestimation of zfs. It is therefore important than any employed model be as simple as possible. In this respect, we have carried out DFT calculations to estimate the magnitude of the exchange through the shortest inter-molecular contacts between [ReCl6]2− moieties in all six complexes. These values, together with the shortest Re⋯Re, Re⋯Cu, and Cl⋯Cl distances between adjacent chains are collected in Table 1.
Compound | d(Re⋯Re)/Å | d(Re⋯Cu)/Å | d(Cl⋯Cl)/Å | J/cm−1 |
---|---|---|---|---|
1 | 7.87 | 8.05 | 3.80 | −0.023 |
6.87 | +0.000 | |||
2 | 8.18 | 7.71 | 3.86 | +0.027 |
4.29 | +0.004 | |||
3 | 9.22 | 8.83 | 5.425 | +0.001 |
6.55 | +0.000 | |||
6.59 | +0.004 | |||
4 | 10.73 | 9.33 | 7.01 | +0.000 |
7.67 | +0.000 | |||
5 | 8.75 | 9.74 | 4.64 | +0.003 |
6 | 8.46 | 9.49 | 5.22 | +0.007 |
5.34 | +0.006 |
DFT calculations show that the inter-chain magnetic exchange interactions in 1–6 are negligible, even in the cases of complexes 1 and 2 where the Cl⋯Cl contacts are relatively short (Table 1). The magnetic behaviour of 1–6 can therefore be regarded as originating from isolated heterometallic 1D chains.
The magnetic properties of certain homo- and heterometallic ReIV based complexes have previously been studied using an approach that considers only the lowest-lying Kramers doublet is populated at low temperature, rendering the ion an effective spin doublet (Seff = 1/2).5 However, this approach is only useful when DRe ≫ JReCu (by at least one order of magnitude). In most cases involving pseudohalide [ReX6]2− ions this condition is not met, and the analytical methodology required for implementing this approach becomes rather complex.23 In order to verify our starting point, we have therefore performed a NEVPT2 calculation of the axial (D) and rhombic (E) components of the zfs tensor of the [ReCl6]2− ion in complex 1. The results afford g = 1.761, D = −8.0 cm−1, and E/D = 0.163, confirming the presence of a moderate axial component of the magnetic anisotropy (DRe ≈ JReCu). Thus an approach based on the exact diagonalization of the energy matrix of a {ReIVCuII}n wheel, has been employed. The weak magnetic exchange between the metal ions, clearly observed in the susceptibility data, allows us to use a model wheel that incorporates just eight metal centres (Fig. 3). The magnetic coupling between the paramagnetic centres is described as the sum of the Zeeman (ĤZeem), zero-field splitting (Ĥzfs) and Heisenberg magnetic coupling (ĤHeis) contributions, where B is the applied magnetic field and β the Bohr magneton:
The theoretical curves obtained using this spin-Hamiltonian are shown in Fig. 4.5 Positive and negative values for DRe and J were used to identify the effects on the thermal dependence of the magnetic susceptibility. When there is zero coupling between the metal ions the magnetic behaviour does not depend on the sign of the axial zfs parameter, and the χMT value decreases to a non-zero value at T = 0 K (χMT0). If the exchange coupling is non-zero, the magnetic behaviour is affected by the sign of DRe, but only at very low temperatures. For example, when the neighbouring spins are antiferromagnetically coupled, the |±3/2〉 Kramers doublet of the ReIV ion is coupled with the |±1/2〉 doublet of the CuII ion for DRe < 0. In such a scenario, the spins do not cancel and an increase in χMT is observed at low temperatures, leading to values slightly larger than χMT0. For DRe > 0, the spin of the |±1/2〉 ground Kramers doublet on the ReIV ion can be ‘cancelled out’ by coupling to the CuII ion, though the curve is also dependent on the different g-factors. Thus, a continuous decrease of χMT occurs to values lower than the χMT0 limit. When the exchange is ferromagnetic, χMT increases with decreasing temperature, diverging at low temperature towards a non-finite value, as expected for an ideal one-dimensional system. For small J/DRe ratios a small decrease in χMT is observed leading to values at low temperatures that are greater than χMT0.
Fig. 4 Theoretical thermal dependence of the χMT product for the model schematised in Fig. 3 for different values of J and D (inset). The dark red line (J = 0 cm−1, D = +5 cm−1) is directly superimposed on the dark blue line (J = 0 cm−1, D = −5 cm−1). |
We can therefore extract some qualitative conclusions from the experimental thermal dependence of χMT in Fig. 2. The continuous decrease of the χMT value to values close to χMT0 for complexes 2, 4 and 6 suggest that the magnetic coupling in these compounds could be ferro- or antiferromagnetic, but very weak in each case. The higher χMT values at T = 2 K in 2 and 6, suggest these systems possess a small but non-negligible ferromagnetic coupling. The greater decrease in χMT in 4 indicates the presence of antiferromagnetic exchange, whilst the sharp increase in χMT at low temperatures in 1, 3 and 5 is evidence of ferromagnetic exchange interactions. The minimum in the χMT value close to the χMT0 limit observed in 1 points to a smaller J/DRe ratio than detected in 3 and 5.
In order to support these qualitative conclusions, and to establish which structural parameters govern the nature and magnitude of the magnetic exchange coupling (Fig. 5), we have theoretically estimated J from DFT calculations on a [ReIVCuII2] fragment (Table 2 and Fig. S15†). We note the following points: (a) complexes 1 and 2 each contain two distinct coupling constants (derived from two different geometries), assigned X_1 and X_2; (b) two different ReIVCuII chains coexist in 2, named 2a and 2b; the exchange is weak and mediated via the axial JT axis of the CuII ion. Thus the results should be regarded as semi-quantitative with some leeway allowed for the estimated J values.
Fig. 5 Perpendicular (left) and parallel (right) views of the Jahn–Teller axis of the CuII ion in a ReIVCuII fragment, highlighting the Cu–Cl distance (d(Cu–Cl)), the Cu–Cl–Re angle (α), and the twist of the ReCl6 moiety around the JT axis of the CuII ion (θ). Colour code as Fig. 1. |
Coupling | d(Cu–Cl)/Å | α/° | θ/° | J/cm−1 |
---|---|---|---|---|
1_1 | 3.058 | 148.59 | 41.68 | −0.37 |
1_2 | 2.993 | 152.79 | 26.41 | +0.57 |
2a | 3.045 | 146.71 | 19.92 | +0.29 |
2b_1 | 3.195 | 143.60 | 43.42 | +0.64 |
2b_2 | 3.038 | 140.03 | 42.68 | +0.71 |
3 | 2.883 | 132.99 | 9.43 | +2.38 |
4 | 3.226 | 142.25 | 8.22 | +0.31 |
5 | 2.857 | 128.66 | 39.15 | +2.53 |
6 | 2.780 | 142.92 | 17.35 | +0.68 |
As predicted from the theoretical simulations (Fig. 4), the strongest ferromagnetic exchange interactions are observed in complexes 3 and 5 (Table 2). Ferromagnetic and antiferromagnetic exchange co-exists in 1, the former stronger than the latter, in agreement with the observed experimental data. The weakest interactions in the family are observed in 2 and 4. The average value of J in 2 is consistent with the experimental data, showing a tendency for χMT to increase at temperatures close to T = 2 K. A comparison of the J values with the Re–Cl–Cu bond angle, α, shows the coupling to become more ferromagnetic with a smaller bridging angle (Fig. S16†). As expected, the second-neighbouring Cu–Cu magnetic coupling is zero in all calculated [ReIVCuII2] fragments.
In order to establish a magneto-structural correlation for this family of complexes we have examined how the strength of the exchange varies with the Cu–Cl distance (d(Cu–Cl)), the Cu–Cl–Re angle (α), and the twist of the [ReCl6]2− moiety around the JT axis of the CuII ion (θ), using the model complex shown in Fig. 5. The d(Cu–Cl) bond length and the α and θ angles have been varied between 2.50–3.25 Å, 125 to 155°, and 0–45°, respectively. The results are summarized in the 2D contour maps shown in Fig. 6 and S17–S19.† The results confirm our previous conclusions: (1) the magnetic exchange is weak in all cases; (2) they are mainly ferromagnetic in nature; (3) the magnitude of the coupling strongly depends on the α angle, but only slightly on the θ angle; (4) the axial Cu–Cl bond length strongly modifies the magnitude of the magnetic coupling; the shorter the bond the stronger the exchange. This last point is clear from Fig. 7 for two pairs of α and θ values.
Fig. 6 Contour maps of the dependence of the α and θ angle on the magnetic coupling constant in the molecular model of Fig. 5 for several Cu–Cl bond lengths in the range 2.50–2.75 Å at regular intervals of 0.25 Å. The J value (cm−1) range is indicated by the colour graded bar. |
Fig. 7 Dependence of the Cu–Cl bond length on the magnetic coupling for the geometries ({α, θ}) {125°, 45°} (blue) and {155°, 45°} (red). |
The CuII ion has a unique magnetic orbital on its basal plane (dx2−y2), with the ReIV ion having all three t2g orbitals half-filled. Of these, the dxz and dyz magnetic orbitals delocalize their spin densities to the px and py orbitals of the bridging chloride ion; the dxy magnetic orbital does not. The former are therefore the only magnetic orbitals to interact with the magnetic orbital of the CuII ion. A schematic evolution of this interaction is shown in Fig. 8. From this picture, it is clear to see that the contribution caused by the interaction between the dxz orbital on the ReIV ion and the dx2−y2 orbital on the CuII ion should be ferromagnetic, and invariant with α (Fig. 8).24,25
Because of zero orbital overlap, the contribution promoted by the dyz magnetic orbital should also be ferromagnetic. For smaller angles of θ this contribution should become larger, due to the increased interaction between the spin densities on the magnetic orbitals, despite orbital overlap remaining zero. The strong dependence of the Cu–Cl bond length on the magnetic exchange is clear from Fig. 7, and can be understood by a decrease in the interaction between the spin densities when this distance increases. Thus complexes 3 and 5 exhibit the strongest ferromagnetic coupling. Note that the theoretical exchange couplings are slightly more ferromagnetic than the experimental ones.
With the theoretical study as a guide, we then attempted to use our model to fit the experimental susceptibility data (Fig. 2), and obtained good simulations with the set of parameters given in Table 3. The analysis for compound 1 was excluded due to the presence of multiple coupling pathways. The experimental behaviour is in agreement with the calculated magnetic coupling constants, and the J values in Table 3 agree well with those in Table 2 and Fig. 9.
Fig. 9 The magnetic exchange parameters versus Re–Cl–Cu bridging angle. Points labelled in accordance with Table 3. Grey dots correlate to the values presented in Table 2. |
Compound | g Re | D Re/cm−1 | g Cu | J/cm−1 |
---|---|---|---|---|
2 | 1.804 | −15.8 | 2.050 | +0.11 |
3 | 1.778 | −9.1 | 2.054 | +1.59 |
4 | 1.807 | −13.1 | 2.070 | −0.12 |
5 | 1.764 | −16.5 | 2.115 | +2.16 |
6 | 1.814 | −6.8 | 2.056 | +0.33 |
Footnote |
† Electronic supplementary information (ESI) available: Crystallographic, structural and magnetic data. CCDC 1550271–1550276. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c7dt02216f |
This journal is © The Royal Society of Chemistry 2017 |