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. 2022 Jan 27;17(5):e202101328. doi: 10.1002/asia.202101328

Lanthanoid Biphenolates as a Rich Source of Lanthanoid‐Main Group Heterobimetallic Complexes

Safaa H Ali 1, Angus C G Shephard 1, Jun Wang 1, Zhifang Guo 1, Murray S Davies 1, Glen B Deacon 2, Peter C Junk 1,
PMCID: PMC9303937  PMID: 35034432

Abstract

Several new trivalent dinuclear rare earth 2,2’‐methylenebis(6‐tert‐butyl‐4‐methylphenolate) (mbmp2−) complexes with the general form [Ln2(mbmp)3(thf)n] (Ln=Sm 1, Tb 2 (n=3), and Ho 3, Yb 4 (n=2), and a tetravalent cerium complex [Ce(mbmp)2(thf)2] (5) have been synthesised by RTP (redox transmetallation/protolysis) reactions from lanthanoid metals, Hg(C6F5)2 and the biphenol mbmpH2. These new complexes and some previously reported partially protonated rare earth biphenolate complexes [Ln(mbmp)(mbmpH)(thf)n] react with lithium, aluminium, potassium and zinc organometallic reagents to form lanthanoid‐main group heterobimetallic species. When reaction mixtures containing the Ln biphenolate complexes were treated with n‐butyllithium, both molecular ([Li(thf)2Ln(mbmp)2(thf)n] (Ln=La 6, Pr 7 (n=2) and Er 8, Yb 9, and Lu 10 (n=1)) and charge separated ([Li(thf)4][Ln(mbmp)2(thf)2] (Ln=Y 11, Sm 12, Dy 13, and Ho 14) complexes were isolated. Treatment with trimethylaluminium also led to isolation of molecular ([AlMe2Ln(mbmp)2(thf)2] (Ln=Pr 15, Sm 16, and Tb 17)) and ionic [La(mbmp)(thf)5][AlMe2(mbmp)] (18) complexes. One gadolinium‐potassium ([K(thf)3Gd(mbmp)2(thf)2] (19)), and one ytterbium‐zinc species ([ZnEtYb(mbmp)2(thf)] (20)) were isolated from treatment of reaction mixtures with potassium bis(trimethylsilyl)amide and diethylzinc respectively.

Keywords: biphenolate ligands, coordination chemistry, heterobimetallic complexes, rare earth complexes, redox transmetallation


Trivalent dinuclear rare earth 2,2′‐methylenebis(6‐tert‐butyl‐4‐methylphenolate) (mbmp2‐) complexes with the general form [Ln2(mbmp)3(thf)n] react with lithium, aluminium, potassium and zinc organometallic reagents to form lanthanoid‐main group heterobimetallic species.

graphic file with name ASIA-17-0-g014.jpg

Introduction

Lanthanoid alkoxide and aryloxide complexes have garnered significant attention in the field of coordination chemistry in recent years, [1] particularly as bulky ligands for low coordinate rare earth complexes.[ 1 , 2 , 3 ] The popularity of carbon bridged biphenolate ligands has stemmed from their tunability, their ability to chelate to a metal centre reducing the potential for redistribution reactions, as well as offering a rigid framework for the metal centre, potentially affecting stereospecific transformations. Alongside this, lanthanoid biphenolate complexes have applications in sol gel methods, [1] as feedstocks in MOCVD and ALD deposition of oxide layers, [4] and as catalysts for ring opening polymerisation of cyclic esters. [5] These biphenolate complexes have previously been synthesised by halide metathesis, or protolysis/ligand exchange reactions.[ 6 , 7 , 8 , 9 , 10 , 11 ] We have previously described the synthesis of a range of lanthanoid phenolate complexes using 2,2’‐methylenebis(6‐tert‐butyl‐4‐methylphenol) (mbmpH2) (Figure 1), utilising a redox transmetallation/protolysis (RTP) approach[ 12 , 13 ] from free rare earth metals, bis(pentafluorophenyl)mercury and mbmpH2 to yield partially deprotonated lanthanoid biphenolate complexes. [14] Herein, we describe the synthesis and structures of new lanthanoid biphenolate complexes of the type [Ln2(mbmp)3(thf)n] by RTP reactions, and the facile ability of these complexes to form lanthanoid‐main group heterobimetallic complexes with lithium, aluminium, potassium, and zinc.

Figure 1.

Figure 1

2,2’‐methylenebis(6‐tert‐butyl‐4‐methylphenol) (mbmpH2)

Results and discussion

Synthesis and Characterisation of Lanthanoid Biphenolate Complexes

The RTP reaction was used in this study to provide a simple, accessible synthetic method for a range of lanthanoid biphenolate complexes.

We have previously described a similar synthetic approach to yield mononuclear, partially deprotonated rare earth biphenolate complexes with the general form [Ln(mbmp)(mbmpH)(thf)3] (Ln=Y, Nd, Gd, Dy, Er Tm and Lu), [14] by using an mbmpH2:RE metal:Hg(C6F5)2 ratio of 4 : 3 : 3 respectively (metal was used in excess) (Scheme 1 (a)). We now report a range of fully deprotonated trivalent dinuclear complexes, of the general form [Ln2(mbmp)3(thf)n] (Ln=Sm 1, Tb 2 (n=3) and Ho 3, Yb 4 (n=2)) (Scheme 1 (b)), and a tetravalent mononuclear cerium complex [Ce(mbmp)2(thf)2] 5 (Scheme 1 (c)). Reactions were undertaken in thf at room temperature for 3 days, with a drop of Hg metal to activate the lanthanoid metal, leading to the isolation of complexes 15 as crystals from concentrated solutions. It is noteworthy that 14 with doubly deprotonated ligands and the previously reported [Ln(mbmp)(mbmpH)(thf)3] complexes preferentially crystallised after similar synthesis conditions with no evidence of mixtures. The selectivity is not due to lanthanoid ion size, and perhaps solubility is a key factor.

Scheme 1.

Scheme 1

RTP reactions between mbmpH2, free rare earth metals and Hg(C6F5)2. All reactions performed in anhydrous thf at room temperature.

Satisfactory microanalyses and complexometric Ln analyses were obtained for 14, generally showing loss of solvent of crystallization from the crystal composition, as the analysis samples were dried under reduced pressure. All the Ln3+ ions in the complexes are paramagnetic and satisfactory 1H NMR spectra could not be obtained. Complex 5 was obtained only in an amount sufficient for X‐ray crystallographic identification. It is known, having been identified by crystallography, as a component of a mixture from several oxidation reactions of [Li(thf)2Ce(mbmp)2(thf)2]. [15] The infrared spectra of complexes 14 are consistent with complete deprotonation of mbmpH2 as the v(OH) bands of the biphenol (ca. 3600 cm−1 and 3390 cm−1) are absent.

Structures of 1–5

X‐ray crystal structures were determined for 15 and selected bond lengths of these complexes have been summarised below with the appropriate structural figures.

Complexes 1 and 2 are isostructural with a previously reported dinuclear dysprosium complex. [14] The Ln(1) atom is six‐coordinate, with distorted octahedral stereochemistry (Figure 2), and is coordinated by two bridging bidentate mbmp2− ligands (O1,2; O3,4), and two cis thf molecules (O(7)‐Ln(1)‐O(8) 94.22(17)° (1) and 92.08(9)° (2)). The Ln(2) atom is five‐coordinate, with a distorted square pyramidal donor array. It is equatorially ligated by a single oxygen (O2,4) of two bridging mbmp2− ligands, one equatorial chelating mbmp2− (O5,6) and one axial thf molecule.

Figure 2.

Figure 2

ORTEP diagram of complex 1 (also representative of 2) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths of 1 (with data for 2 in square brackets) (Å): Ln(1)‐O(1) 2.218(5) [2.192(2)], Ln(1)‐O(2) 2.358(5) [2.291(2)], Ln(1)‐O(3) 2.211(5) [2.188(2)], Ln(1)‐O(4) 2.353(5) [2.361(2)], Ln(1)‐O(7) 2.496(5) [2.425(3)], Ln(1)‐O(8) 2.504(6) [2.421(2)], Ln(2)‐O(2) 2.375(5) [2.350(2)], Ln(2)‐O(4) 2.356(5) [2.332(2)], Ln(2)‐O(5) 2.144(5) [2.119(2)], Ln(2)‐O(6) 2.145(5) [2.108(2)], Ln(2)‐O(9) 2.458(6) [2.448(2)].

Complexes 3 and 4 are isostructural, and the composition varies from complexes 1 and 2 by one less coordinated thf molecule. Both metal atoms have a distorted square pyramidal stereochemistry (Figure 3). Ln(1) is coordinated by two bridging, bidentate mbmp2− ligands, with O(1) and O(3) terminal, and O(2) and O(4) bridging to Ln(2), and a thf donor. The other metal atom, Ln(2), is coordinated by the bridging oxygens, a terminal, chelating mbmp2− ((O(5) and O(6)), and a thf molecule.

Figure 3.

Figure 3

ORTEP diagram of complex 3 (also representative of 4) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths of 3 (with data for 4 in square brackets) (Å): Ln(1)‐O(1) 2.078(3) [2.062(5)], Ln(1)‐O(2) 2.259(3) [2.242(5)], Ln(1)‐O(3) 2.104(3) [2.035(5)], Ln(1)‐O(4) 2.248(3) [2.203(5)], Ln(1)‐O(7) 2.353(5) [2.317(5)], Ln(2)‐O(2) 2.270(3) [2.218(5)], Ln(2)‐O(4) 2.287(3) [2.245(5)], Ln(2)‐O(5) 2.081(3) [2.066(5)], Ln(2)‐O(6) 2.081(3) [2.052(5)], Ln(2)‐O(8) 2.382(3) [2.365(5)].

Complex 5 is comprised of a six‐coordinate cerium centre, with a distorted octahedral donor array (Figure 4). The cerium atom is coordinated by two chelating mbmp2− ligands, and two cis thf molecules. The metrical parameters agree with those reported. [15]

Figure 4.

Figure 4

ORTEP diagram of complex 5 showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths (Å): Ce(1)‐O(1) 2.153(3), Ce(1)‐O(2) 2.130(3), Ce(1)‐O(3) 2.113(3), Ce(1)‐O(4) 2.147(3), Ce(1)‐O(5) 2.507(4), Ce(1)‐O(6) 2.522(4).

Reactions to form Heterobimetallics

Lanthanoid biphenolate heterobimetallic chemistry is still limited and few complexes have been reported. We previously reported the synthesis of an yttrium‐aluminium bimetallic complex from treating the partially protonated yttrium biphenolate complex [Y(mbmp)(mbmpH)(thf)3] with trimethylaluminium, [14] and the Yb analogue was previously prepared by the same method. [7] We have since expanded this approach to synthesise a range of new rare earth heterobimetallics with lithium, aluminium, potassium, and zinc. An Sm−Al mbmp tetramethylaluminate complex has previously been prepared by protolysis of [Sm(AlMe4)3] with mbmpH2 and was treated with azobenzene to give a dimethylaluminum derivative. [16] Other molecular rare earth‐potassium heterobimetallic biphenolate complexes, namely of Sm and Yb have previously been synthesised by metathesis reactions of mbmpK2 with the corresponding rare earth chloride. [11]

Reactions with n–butyllithium

When RTP reaction mixtures (a) for the formation of 1, 3, and 4 or (b) for the formation of [Ln(mbmp)(mbmpH)thf)3] (Ln=Dy, Y, Er, Lu) or (c) for the formation of putative La and Pr analogues which so far have not been crystallised, were treated with n‐butyllithium (Ln : Li=1 : 1), heterobimetallic complexes 614 were successfully obtained (Scheme 2 (a)‐(c) respectively). Irrespective of the synthetic route, the resulting heterobimetallic was either molecular (complexes 610), or a discrete cation‐anion pair (complexes 1114). Elemental analyses of the complexes were determined after drying under reduced pressure, and therefore some exhibited loss of lattice solvent and in some cases coordinated solvent from the crystal composition as determined by X‐ray crystallography. Thus, microanalyses of 6 and 7, which have no lattice solvent, corresponded to the crystal composition. Complex 8 exhibited loss of two lattice C6D6 and two coordinated thf, 10 loss of three C6D6 lattice solvent, 11 loss of one lattice thf and two coordinated thf, 12 and 13 exhibited loss of 0.5 lattice thf, and 14 exhibited loss of one lattice thf and four coordinated thf molecules. These results were supported by complexometric titration to determine the % rare earth metal. Crystals of complex 9 were isolated, but only in low yields, hence only an X‐ray crystal structure could be obtained.

Scheme 2.

Scheme 2

Reactions of in situ formed (a) dinuclear and (b) mononuclear partially deprotonated rare earth biphenolate complexes with n‐butyllithium to form heterobimetallics. All reactions were performed in anhydrous thf at room temperature.

IR spectra of complexes 614 are consistent with complete deprotonation of the mbmpH2 starting material (no v(OH) absorption). Of these complexes only the 1H NMR spectra of 6 and 10 were able to be recorded and interpreted, and both confirm biphenolate:thf ratios observed in the X‐ray crystal structures. The molecular Li/Ln complexes show the bridging CH2 resonance split into an apparent AB doublet (slightly broadened in the case of 10).

Complexes 6 and 7 are isomorphous (Table S1) molecular compounds and are comprised of a six‐coordinate, distorted octahedral Ln atom, bridged by phenolate oxygen atoms to a four‐coordinate, distorted tetrahedral Li atom (Figure 5). The Ln atom is bound by two mbmp2− ligands (O1,2 and symmetry equivalent), with one oxygen of each bound solely to the Ln atom in the axial positions, and the other oxygen of each bridging between the Ln and the Li atoms, and two cis thf molecules in the equatorial sites. The Li atom is bound by two bridging mbmp2− oxygens, and two thf molecules. The bridging oxygens of the two mbmp2− ligands have considerably longer Ln−O bond lengths than their non‐bridging counterparts.

Figure 5.

Figure 5

ORTEP diagram of complex 6 (also representative of 7) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths of 6 (with data for 7 in square brackets) (Å): Ln(1)‐O(1) 2.3408(16) [2.267(5)], Ln(1)‐O(2) 2.3948(15) [2.366(5)], Ln(1)‐O(3) 2.5989(18) [2.581(5)], Li(1)‐O(2) 1.969(4) [1.887(15)], Li(1)‐O(4) 2.020(4) [1.99(2)].

Complexes 810 are isostructural molecular compounds and are comprised of a five‐coordinate, distorted square pyramidal Ln atom, linked to a four‐coordinate, distorted tetrahedral Li atom (Figure 6). Similar to complexes 6 and 7, the Ln centre is coordinated by two mbmp2− ligands (O1,2 and O3,4), each with one terminal oxygen, and one oxygen bridging the Ln and Li atoms, and one thf. The two bridging mbmp2− oxygens, and two molecules of thf ligate the Li atom. Again, the bridging Ln−O bond lengths are considerably longer than their non‐bridging counterparts. A previously prepared Yb−Li analogue [7] is isostructural and differs only in the associated lattice solvent (1 PhMe and 0.5thf) [7] vs hexane (Table S1).

Figure 6.

Figure 6

ORTEP diagram of complex 8 (also representative of 9 and 10) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths of 8 (with data for 9 and 10 respectively in square brackets) (Å): Ln(1)‐O(1) 2.1097(16) [2.070(19), 2.0724(19)], Ln(1)‐O(2) 2.1711(18) [2.2068(18), 2.1502(17)], Ln(1)‐O(3) 2.0763(17) [2.080(2), 2.0475(18)], Ln(1)‐O(4) 2.2434(15) [2.1552(18), 2.1613(17)], Li(1)‐O(2) 2.004(5) [1.943(5), 1.993(5)], Li(1)‐O(4) 1.957(4) [2.031(5), 1.984(5)], Ln(1)‐O(5) 2.3598(18) [2.3454(19), 2.3213(19)], Li(1)‐O(6) 1.969(5) [2.031(5), 1.966(5)], Li(1)‐O(7) 1.993(4) [1.974(5), 2.009(4)].

Complexes 1114 are isostructural ionic compounds, with a six‐coordinate, octahedral Ln atom in the anion, and a four‐coordinate, tetrahedral Li atom in the cation (Figure 7). The Ln centre is bound by two fully deprotonated mbmp2− ligands, and two cis thf molecules (e. g. O(5)‐Sm(1)‐O(6)=82.46(7)°) in the equatorial positions. The Ln−O bonds of the mbmp2− ligands are considerably longer in the axial positions. The [Li(thf)4]+ cation is widely reported in the literature, with 595 structural studies. [17] Similar ionic rare earth‐lithium biphenolate/amide heterobimetallics with the general form [Li(thf)4][Ln(mbmp)(N(SiCH3)3)2] (Ln=Nd and Yb) have previously been synthesised by treatment of chloride bridged rare earth biphenolate complexes with lithium bis(trimethylsilyl)amide, [18] where the [Li(thf)4]+ cation shows slightly longer Li‐O(thf) bond lengths (average Li‐O(thf)=1.908 Å) than complexes 1114 (average Li‐O(thf)=1.845 Å). The difference in bond length could be attributed to elevated temperatures during data collection for the [Li(thf)4][Ln(mbmp)(N(SiCH3)3)2] compounds (193 K vs 100 K for 1114).

Figure 7.

Figure 7

ORTEP diagram of complex 11 ((a)=[Li(thf)4]+ and (b)=[Ln(mbmp)2(thf)2]) (also representative of 12–14) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths have been summarised in Table 1. Selected bond lengths of 11 (with data for 12–14 respectively in square brackets)(Å): Ln(1)‐O(1) 2.121(3) [2.2595(17), 2.207(2), 2.201(2)], Ln(1)‐O(2) 2.183(4) [2.176(2), 2.144(3), 2.125(3)], Ln(1)‐O(3) 2.207(4) [2.2137(17), 2.175(2), 2.160(2)], Ln(1)‐O(4) 2.131(4) [2.2718(17), 2.213(2), 2.213(2)], Ln(1)‐O(5) 2.438(3) [2.513(2), 2.453(3), 2.439(3)], Ln(1)‐O(6) 2.438(4) [2.523(2), 2.459(2), 2.444(2)].

Just as there was no obvious correlation between which Ln elements form [Ln(mbmp)(mbmpH)(thf)n] and which give [Ln2(mbmp)3(thf)n] complexes in RTP reactions, the factors deciding which Ln metals give molecular Li/Ln bimetallics (La, Pr, Y, Er, Yb, Lu) and which give charge separated species (Sm, Dy, Ho) are not clear. Whilst the latter appear associated with mid‐sized Ln3+, a break between Ho and Y/Er is surprising. The division cannot be correlated with the two different classes of reagent, as some from each class fall into each class of heterobimetallics. Moreover, the molecular/ charge separated division for Li/Ln bimetallics does not relate to the division within Al/Ln bimetallics (below) where La and Pr fall into different classes and Sm now gives a molecular Al/Sm species. It may be that solubilities and crystallization conditions decide the outcome.

Reactions with trimethylaluminium

Several rare earth‐aluminium heterobimetallics were synthesised in a similar fashion to the rare earth‐lithium heterobimetallics: namely by treatment of the RTP reaction mixtures containing the dinuclear complexes [Ln2(mbmp)3(thf)n] (from reaction of mbmpH2 with La, Pr, Sm and Tb metals and Hg(C6F5)2) with trimethylaluminium (Al: Ln=1 : 1; Scheme 3). This method yielded either molecular rare earth‐aluminium heterobimetallics with the general form [AlMe2Ln(mbmp)2(thf)] (Ln=Pr (15), Sm (16), and Tb (17)), or a discrete cation‐anion pair in [AlMe2(mbmp)][La(mbmp)(thf)4] (18) (Scheme 3).

Scheme 3.

Scheme 3

Reactions of dinuclear rare earth complexes with trimethylaluminium to yield heterobimetallics. *The precursors of complexes 15 and 18 could not be isolated. All reactions were performed in anhydrous thf at room temperature.

Elemental analyses were collected after drying under reduced pressure. Complex 15 exhibited loss of two lattice C6D6, 16 exhibited loss of one and half lattice C6D6 and one coordinated thf, 17 loss of two lattice C6D6, and 18 exhibited loss of three coordinated thf molecules. These results were supported by complexometric titration to determine the % Ln. In the IR spectra of complexes 1518 no v(OH) absorptions were observed signifying total deprotonation of the mbmpH2 ligand. The 1H NMR spectrum of paramagnetic 17 was able to be collected and interpreted, confirming biphenolate:thf:Me(Al) ratios. Complex 17 also shows the splitting of the bridging CH2 resonance observed for the Li/Ln heterobimetallics, but this feature is shifted to lower energies, whereby one of the signals is slightly masked by the thf resonance.

Complexes 1517 are isostructural molecular compounds, comprised of a six‐coordinate, distorted trigonal prismatic Ln atom, linked to a four‐coordinate, distorted tetrahedral Al atom (Figure 8). Ln(1) is coordinated by two bridging mbmp2− ligands, and two transoid thf molecules (O(5)‐Ln(1)‐O(6)=149.45(13)° (15), 148.71(10)° (16), 150.1(2)° (17)). One oxygen of each mbmp2− ligand is coordinated solely to the Ln, whilst the other is bridging between the Ln and Al atoms. The aluminium atom is coordinated by the two bridging mbmp2− oxygens, and two methyl groups. Again, the Ln−O bond lengths of the bridging oxygens are significantly longer than their non‐bridging counterparts. Analogous rare earth‐aluminium biphenolate bimetallics with the general form [AlMe2Ln(mbmp)2(thf)2] (Ln=Y, [14] and Sm [16] ) have been reported, the former from reaction of an isolated [Y(mbmp)(mbmpH)(thf)3] complex and there are analogous lanthanum‐ and cerium‐aluminium based anilido complexes. [19]

Figure 8.

Figure 8

ORTEP diagram of complex 15 (also representative of 16 and 17) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths of 15 (with data for 16 and 17 respectively in square brackets) (Å): Ln(1)‐O(1) 2.119(4) [2.162(3), 2.188(6)], Ln(1)‐O(2) 2.507(4) [2.447(3), 2.515(6)], Ln(1)‐O(3)2.171(4) [2.143(3), 2.493(6)], Ln(1)‐O(4)2.497(4) [2.447(3), 2.162(6)], Ln(1)‐O(5) 2.533(4) [2.466(3), 2.527(7)], Ln(1)‐O(6) 2.561(4) [2.475(3), 2.557(6)], Al(1)‐O(2)1.817(4) [1.829(3), 1.835(6)], Al(1)‐O(4)1.830(4) [1.833(3), 1.838(6)], Al(1)‐C(55) 1.982(8) [1.969(5), 1.976(12)], Al(1)‐C(56) 1.927(9) [1.970(5), 1.969(11)].

Complex 18 is an ionic compound, comprised of a seven‐coordinate, distorted pentagonal bipyramidal lanthanum cation and a four‐coordinate, distorted tetrahedral aluminium anion (Figure 9). The lanthanum atom is ligated by one mbmp2− ligand, one oxygen in an axial, and the other in an equatorial position (O(1)‐La(1)‐O(2)=92.93(7)°) and five thf molecules, one in an axial, and four in equatorial positions. The aluminium atom is ligated by two methyl groups, and one chelating mbmp2− ligand.

Figure 9.

Figure 9

ORTEP diagram of complex 18 ((a)=[La(mbmp)(thf)5]+ and (b)=[AlMe2(mbmp)]) showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths (Å): La(1)‐O(1) 2.2282(19), La(1)‐O(2) 2.2460(19), Al(1)‐O(8) 1.765(2), Al(1)‐O(9) 1.785(2), La(1)‐O(3) 2.595(2), La(1)‐O(4) 2.609(2), La(1)‐O(5) 2.598(2), La(1)‐O(6) 2.638(3), La(1)‐O(7) 2.572(2).

A reaction with potassium bis(trimethylsilyl)amide

One rare earth‐potassium heterobimetallic complex was isolated, which was from the reaction of [Gd(mbmp)(mbmpH)(thf)3] [14] with one equivalent of KN(SiMe3)2, yielding [K(thf)3Gd(mbmp)2(thf)2] (19) (Scheme 4). The IR spectrum of 19 shows complete deprotonation of the mbmpH2 ligand by the absence of a v(OH) band. An interpretable 1H NMR spectrum could not be collected due to the paramagnetic nature of Gd3+. The elemental analysis of 19 after drying under vacuum showed loss of one half of a lattice thf molecule, and this was supported by complexometric titration to determine % Gd.

Scheme 4.

Scheme 4

Reaction of a partially protonated, mononuclear Gd complex with potassium bis(trimethylsilyl)amide to yield a Gd−K bimetallic complex (19).

Complex 19 consists of a six‐coordinate, octahedral gadolinium atom linked to a five‐coordinate, distorted square pyramidal potassium atom (Figure 10). The gadolinium atom is ligated by two bridging mbmp2− ligands, and two cis equatorial thf molecules (O(5)‐Gd(1)‐O(6)=94.81(16)°). One oxygen of each mbmp2− ligand is coordinated solely to the Gd, whilst the other is bridging between the Gd and K atoms. The potassium atom is ligated by three thf molecules, and two bridging mbmp2− oxygens. Since this is a low coordination number for the large potassium ion, we have investigated adjacent carbon and hydrogen atoms for the possibility that they ae are contributing electron density to the potassium atom (Table 1 and Figure 11). From consideration of K−C bond lengths in K(η6 –arene) + complexes, K−C distances of <3.5 Å can be considered an interaction [20] and from a range of other structures, K−H may be interacting.[ 21 , 22 , 23 , 24 ] On this basis an ipso and an ortho carbon from each mbmp2− ligand, can be considered to interact with potassium, but the conclusion has to be tempered by the role of the binding of the phenolate oxygen in bringing the carbon atoms near K. Likewise, one C−H of each methylene could make an agostic interaction. On the other hand, the second methylene C−H and the closest H of the tBu group are too distant to be considered an interaction. Overall, there are a collection of nearby C and H atoms that can provide additional electron density to K whilst some of the groups also provide steric stabilisation.

Figure 10.

Figure 10

ORTEP diagram of complex 19 showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths (Å): Gd(1)‐O(1) 2.228(5), Gd(1)‐O(2) 2.170(5), Gd(1)‐O(3) 2.210(5), Gd(1)‐O(4) 2.233(5), Gd(1)‐O(5) 2.572(4), Gd(1)‐O(6) 2.515(4), K(1)‐O(2) 2.787(5), K(1)‐O(4) 2.787(5), K(1)‐O(7) 2.695(14), K(1)‐O(8) 2.724(18), K(1)‐O(9) 2.916(16).

Table 1.

Summary of agostic K−C and K−H interactions

Bond

Bond distance [Å]

K−C of accompanying carbon [Å]

K(1)‐C(18)

3.369(5)

K(1)‐C(13)

3.324(5)

K(1)‐C(41)

3.211(5)

K(1)‐C(36)

3.480(6)

K(1)‐H(46B)

3.0534(18)

3.800(8)

K(1)‐H(12 A)

2.8893(17)

3.382(5)

K(1)‐H(12B)

3.3630(17)

3.382(5)

K(1)‐H(35 A)

2.8039(17)

3.339(6)

K(1)‐H(35B)

3.2488(16)

3.339(6)

Figure 11.

Figure 11

Agostic interactions of 11 showing atom‐numbering scheme for atoms involved in Table 1. Coordinated thf and hydrogen atoms not involved in the coordination sphere of K are omitted for clarity.

As observed previously, the Ln−O bond lengths of the bridging oxygens are considerably longer than their non‐bridging counterparts.

A reaction with diethylzinc

Previous attempts of synthesising rare earth‐zinc biphenolate heterobimetallic complexes, by treatment of partially protonated rare earth biphenolates ([Ln(mbmp)(mbmpH)(thf)2] (Ln=Y, and Yb)) with diethylzinc resulted in redistribution, yielding a zinc biphenolate complex, [Zn(mbmp)2(thf)]2 instead of the targeted heterobimetallic. [7] However, when complex 4 was treated with two equivalents of diethylzinc in the presence of one equivalent of mbmpH2, [ZnEtYb(mbmp)2(thf)] (20) was isolated (Scheme 5). The IR spectrum of 20 displayed no v(OH) absorption, confirming complete deprotonation of mbmpH2. Yb3+ is paramagnetic in nature and no interpretable 1H NMR spectrum of 20 could be collected. The elemental analysis after drying under vacuum showed loss of one and a half lattice C6D6 molecules (out of two in the single crystal composition).

Scheme 5.

Scheme 5

Reaction of a dinuclear Yb complex (4) with diethylzinc yielding an Yb−Zn bimetallic complex (20).

Complex 20 is made up of a five‐coordinate ytterbium atom in a distorted square pyramidal geometry, and a three‐coordinate zinc atom in a distorted trigonal planar geometry (Figure 12). The ytterbium atom is bound by two bridging mbmp2− ligands, and one thf molecule. One oxygen of each mbmp2− ligands is coordinated solely to the Yb, whilst the other is bridging between the Yb and Zn atoms. The latter also has an ethyl group bound to it, giving Zn a coordination number of three. The bridging Zn−O bond lengths are similar to those of [Zn(mbmp)(thf)]2. [7]

Figure 12.

Figure 12

– ORTEP diagram of complex 20 showing atom‐numbering scheme for relevant atoms. Thermal ellipsoids are drawn at the 50% probability level. Hydrogen atoms are omitted for clarity. Selected bond lengths (Å): Yb(1)‐O(1) 2.049(5), Yb(1)‐O(2) 2.215(6), Yb(1)‐O(3) 2.031(4), Yb(1)‐O(4) 2.246(7), Zn(1)‐O(2) 1.976(6), Zn(1)‐O(4) 1.961(8), Yb(1)‐O(5) 2.302(6), Zn(1)‐C(51) 1.962(13)

Conclusions

A variety of dinuclear rare earth biphenolate complexes of the general form [Ln2(mbmp)3(thf)n] (Ln=Sm 1, Tb 2 (n=2) and Ho 3, Yb 4 n=3), alongside one previously reported cerium(IV) complex [Ce(mbmp)2(thf)2] (5), have been synthesised by RTP reactions between free Ln metals, Hg(C6F5)2, and mbmpH2. These dinuclear complexes, as well as some known partially protonated [Ln(mbmp)(mbmpH)(thf)n] complexes, generated in situ, were treated with various organometallic bases (lithium, aluminium, potassium and zinc reagents) to yield a range of heterobimetallic complexes. Use of in situ generated complexes greatly simplifies the bimetallic synthesis. Two types of rare earth–lithium bimetallic complexes were obtained, namely molecular compounds with the general form [Li(thf)2Ln(mbmp)2(thf)n] (Ln=La 6, Pr 7 (n=2) and Er 8, Yb 9, and Lu 10 (n=1)) or ionic species with the general form [Li(thf)4][Ln(mbmp)2(thf)2] (Ln=Y 11, Sm 12, Dy 13, and Ho 14). Similarly, treatment with trimethylaluminium led to both molecular compounds with the general form [AlMe2Ln(mbmp)2(thf)2] (Ln=Pr 15, Sm 16, and Tb 17), and an ionic species in the case of lanthanum, [La(mbmp)(thf)5][AlMe2(mbmp)] 18. One each of potassium and zinc heterobimetallic species, namely [K(thf)3Gd(mbmp)2(thf)2] 19 and [ZnEtYb(mbmp)2(thf)] 20 were also isolated from reactions with potassium bis(trimethylsilyl)amide and diethylzinc respectively. The structures of the molecular heterobimetallics feature mbmp2− ligands bridging through one of the phenolate oxygens with the other bound solely to the lanthanoid metal.

Experimental

Materials and General Procedures

All manipulations were performed under nitrogen, using standard Schlenk and drybox techniques. Solvents (thf and toluene) were distilled from sodium benzophenone before use. 2,2’‐Methylene‐bis(6‐tert‐butyl‐4‐methylphenol), n‐butyllithium, trimethylaluminium, and potassium bis(trimethylsilyl)amide, and diethylzinc were commercially available, and used without further purification. Bis(pentafluorophenyl)mercury was prepared by the literature method. [25] Metal analyses were determined by Na2H2edta titration with a Xylenol Orange indicator and hexamethylenetetramine buffer, after decomposition of complexes with dilute HCl. For the heterobimetallic complexes, aluminium was masked in this process by addition of 5% sulfosalicylic acid solution. [26] Infrared spectra (4000–400 cm−1) were obtained as Nujol mulls between NaCl plates with a NicoletNexus FTIR spectrometer. 1HNMR spectra were recorded on a Bruker 400 MHz spectrometer. The chemical shifts were referenced to residual solvent peaks. Crystal data and refinement details are given in Table S1. CCDC 2124516‐2124535 for compound 120, contain the supplementary crystallographic data for this paper. These data can be obtained free of charge from The Cambridge Crystallographic Data Centre via www.ccdc.cam.ac.uk/data_request/cif.

Syntheses

[Sm2(mbmp)3(thf)3] ⋅ 6 thf (1)

A Schlenk flask equipped with a magnetic stirrer bar was charged with mbmpH2 (1.36 g; 4.00 mmol), Hg(C6F5)2 (1.60 g; 3.00 mmol), one drop of Hg metal (to form a reactive lanthanoid‐mercury amalgam) and excess samarium filings (0.45 g; 3.0 mmol). Anhydrous thf (∼20 mL) was added by cannula, and the reaction mixture stirred at room temperature for 3 days. Excess samarium metal and mercury were allowed to settle before isolating the supernatant liquid by a filtration cannula. The resulting filtrate was concentrated under reduced pressure to ∼5 mL and allowed to stand at room temperature to crystallise, yielding colourless crystals (0.40 g, 26%). M. p. 218–220 °C; Anal. Calc. for C81H114O9Sm2 (1532.49 g.mol−1 after loss of six lattice thf): C 63.48, H 7.50, Sm 19.62. Found: C 63.19, H 7.11, Sm 19.14%. IR (Nujol, cm−1): 2058 w, 1750 m, 1249 s, 1138 s, 1060 m, 1011 m, 917 s, 863 s, 814 s, 794 s, 724 m, 670 s.

[Tb2(mbmp)3(thf)3] ⋅ 2 C6D6 (2)

Synthesised as per 1 but with terbium filings (0.47 g, 3.00 mmol) in place of samarium. Colourless crystals grew overnight from C6D6 (0.32 g, 21%) M. p. 243–245 °C; Anal. Calc. for C81H114O9Tb2 (1549.62 g.mol−1 after loss of two lattice C6D6): C 62.78, H 7.42, Tb 20.51. Found: C 62.25, H 7.19, Tb 20.12%. IR (Nujol, cm−1): 1738 w, 1565 m, 1528 w, 1463 s, 1376 s, 1266 s, 1204 m, 1171 w, 1138 m, 1073 m, 1007 s, 913 s, 859 s, 818 s, 789 m, 724 w.

[Ho2(mbmp)3(thf)2] ⋅ 3 C6D6 (3)

Synthesised as per 1 but with holmium filings (0.49 g, 3.00 mmol) in place of samarium. Colourless crystals grew overnight from C6D6 (0.35 g, 24%). M. p. 243–245 °C; Anal. Calc. for C77H106O8Ho2 (1489.52 g.mol−1 after loss of three lattice C6D6): C 62.09, H 7.17, Ho 22.15. Found: C 61.85, H 7.08, Ho 22.06%. IR (Nujol, cm−1): 2284 w, 1936 m, 1854 m, 1795 m, 1747 s, 1600 s, 1570 s, 1260 w, 1208 w, 1003 m, 914 s, 861 s, 819 m, 861 s, 819 m, 777 w, 725 s, 689 m.

[Yb2(mbmp)3(thf)2] ⋅ 1.5 C6D6 (4)

Synthesised as per 1 but with ytterbium filings (0.52 g, 3.00 mmol) in place of samarium. Colourless crystals grew overnight from C6D6 (0.40 g, 27%). M. p. 243–245 °C; Anal. Calc. for C77H106O8Yb2 (1505.77 g.mol−1 after loss of one and a half lattice C6D6) C 61.42, H 7.10, Yb 22.98. Found: C 61.05, H 6.50, Yb 22.45%. IR (Nujol, cm−1): 1943 w, 1738 m, 1569 m, 1259 s, 1120 m, 1093 w, 1023 s, 917 m, 859 s, 798 s, 662 w.

[Ce(mbmp)2(thf)2] ⋅ thf (5)

Synthesised as per 1 but with cerium filings (0.42 g, 3.00 mmol) in place of samarium. Colourless crystals grew after one week from thf (0.05 g, 5%). Owing to the limited yield, no characterisation was obtained other than an X‐ray crystal structure.

[Li(thf)2La(mbmp)2(thf)2] (6)

A Schlenk flask equipped with a magnetic stirrer bar was charged with mbmpH2 (1.36 g; 4.00 mmol), Hg(C6F5)2 (1.60 g; 3.00 mmol), one drop of Hg metal (to form a reactive lanthanoid‐mercury amalgam) and excess lanthanum filings (0.42 g; 3.00 mmol). Anhydrous thf (∼20 mL) was added by cannula, and the reaction mixture stirred at room temperature for 3 days to form either [La(mbmp)(mbmpH)(thf)n] or [La2(mbmp)3(thf)x]. Excess lanthanum metal and mercury were allowed to settle before isolating the supernatant liquid by a filtration cannula. nButylltihium (1.6 M, 0.62 mL, 1.00 mmol) was added to the resulting solution and stirred overnight. The solution was concentrated to ∼5 mL and crystals grew upon standing overnight (0.34 g, 31%). M. p. 228–230 °C; Anal. Calc. for C62H92O8LaLi (1111.24 g.mol−1): 67.01, H 8.34, La 12.50. Found: C 66.71, H 8.02, La 12.30%. 1H‐NMR (400 MHz, C6D6, 25 °C): δ=7.50 (d, 4H, ArH), 7.19 (d, 4H, ArH), 5.03 (d, 2H, CH2), 3.68 (d, 2H, CH2), 3.32 (br, 16H, OCH2, thf), 2.33 (s, 12H, CH3), 1.60 (s, 36H, C(CH3)3), 1.12 (br, 16H, CH2, thf) ppm. IR (Nujol, cm−1): 2667 w, 2390 w, 2110 w, 1744 m, 1605 m, 11462 s, 1372 s, 1258 s, 1200 w, 1025 s, 914 m, 861 m, 808 s, 784 m, 730 s.

[Li(thf)2Pr(mbmp)2(thf)2] (7)

Synthesised as per 6 but with praseodymium filings (0.42 g, 3.00 mmol) in place of lanthanum to form either [Pr(mbmp)(mbmpH)(thf)n] or [Pr2(mbmp)3(thf)x] before treatment with nBuLi. Crystals grew overnight from the mother liquor (0.40 g, 36%). M. p. 168–170 °C; Anal. Calc. for C62H92O8PrLi (1113.24 g.mol−1): C 66.89, H 8.33, Pr 12.66. Found: C 66.17, H 7.69, Pr 12.27%. IR (Nujol, cm−1): 2377 w, 2271 w, 2050 m, 1891 m, 1744 s, 1568 s, 1225 s, 918 s, 861 s, 812 m, 722 m, 669 s.

[Li(thf)3Er(mbmp)2] ⋅ 2 C6D6 (8)

Synthesised as per 6 but with erbium filings (0.50 g, 3.00 mmol) in place of lanthanum to form [Er(mbmp)(mbmpH)(thf)3] before treatment with n‐BuLi. Crystals grew overnight from C6D6 (0.53 g, 57%). M. p. 170–172 °C; Anal. Calc. for C50H68O5ErLi (923.27 g.mol−1 after loss of two coordinated thf and two lattice C6D6): C 65.04, H 7.42, Er 18.12. Found: C 64.72, H 7.06, Er 17.84%. IR (Nujol, cm−1): 2724 s, 2536 w, 2479 w, 2373 w, 2279 w, 2066 m, 1890 m, 1735 s, 1600 s, 1563 m, 1204 w, 1016 m, 922 w, 856 m, 677 m.

[Li(thf)2Yb(mbmp)2(thf)] ⋅ C6H14 (9)

Synthesised as per 6 but with ytterbium filings (0.52 g, 3.00 mmol) in place of lanthanum to form 4 before treatment with nBuLi. A small amount of crystals were grown from a layering of the mother liquor with n‐hexane. No further characterisation could be completed.

[Li(thf)2Lu(mbmp)2(thf)] ⋅ 3 C6D6 (10)

Synthesised as per 6 but with lutetium filings (0.53 g, 3.00 mmol) in place of lanthanum to form [Lu(mbmp)(mbmpH)(thf)3] before treatment with n‐BuLi. Crystals grew overnight from C6D6 (0.54 g, 50%). M. p. 230–232 °C; Anal. Calc. for C58H84O7LuLi (1075.19 g.mol−1 after loss of three lattice C6D6): C 64.79, H 7.87, Lu 16.27. Found: C 64.28, H 7.35, Lu 15.89%. 1H‐NMR (400 MHz, C6D6, 25 °C): δ=7.34 (br s, 4H, ArH), 7.11 (br s, 4H, ArH), 4.69 (d, 2H, CH2), 3.80 (d, 2H, CH2), 3.15 (br, 12H, OCH2, thf), 2.27 (br s, 12H, CH3), 1.60 (s, 36H, C(CH3)3), 1.05 (br, 12H, CH2, thf) ppm. IR (Nujol, cm−1): 2725 w, 2385 w, 2271 m, 1895 w, 1748 s, 1605 s, 1462 s, 1376 s, 1258 m, 1025 m, 861 w, 800 m, 722 m, 673 m.

[Li(thf)4][Y(mbmp)2(thf)2]2 ⋅ 2 thf (11)

Synthesised as per 6 but with yttrium filings (0.27 g, 3.00 mmol) in place of lanthanum to form [Y(mbmp)(mbmpH)(thf)3] before treatment with n‐BuLi. Crystals grew overnight from the mother liquor (0.70 g, 66%). M. p. 132–134 °C; Anal. Calc. for C62H92O8YLi (1061.24 g.mol−1 after loss of two lattice thf and one coordinated thf): C 70.17, H 8.74, Y 8.38. Found: C 69.83, H 8.11, Y 8.05%. IR (Nujol, cm−1): 2370 w, 2275 w, 2049 w, 1883 w, 1741 s, 1605 s, 1381 s, 1254 s, 1204 m, 1172 m, 1139 m, 1025 s, 955 w, 865 s, 788 s, 722 m, 677 m.

[Li(thf)4][Sm(mbmp)2(thf)2] ⋅ 0.5 thf (12)

Synthesised as per 6 but with samarium filings (0.45 g, 3.00 mmol) in place of lanthanum to form 1 before treatment with nBuLi. Crystals grew overnight from the mother liquor (0.54 g, 43%). M. p. 175–177 °C; Anal. Calc. for C70H108O10SmLi (1266.90 g.mol−1 after loss of half of a lattice thf): C 66.36, H 8.59, Sm 11.87. Found: C 66.12, H 7.95, Sm 11.43%. IR (Nujol, cm−1): 2721 m, 2475 w, 2373 m, 2271 m, 2059 m, 1891 s, 1740 s, 1601 s, 1556 s, 1258 w, 1070 w, 874 w, 722 m, 673 s, 583 s.

[Li(thf)4][Dy(mbmp)2(thf)2] ⋅ 0.5 thf (13)

Synthesised as per 6 but with dysprosium powder (0.49 g, 3.00 mmol) in place of lanthanum to form [Dy(mbmp)(mbmpH)(thf)3] before treatment with n‐BuLi. Crystals grew overnight from the mother liquor (0.65 g, 51%). M. p. 200–202 °C; Anal. Calc. for C70H108O10DyLi (1279.04 g.mol−1 after loss of half of a lattice thf): C 65.73, H 8.51, Dy 12.70. Found: C 65.08, H 7.95, Dy 12.19. IR (Nujol, cm−1): 2484 w, 2373 w, 2279 w, 2063 m, 1891 m, 1728 s, 1601 s, 1376 s, 1262 s, 1204 w, 1139 m, 1025 s, 914 m, 861 s, 788 m, 677 m.

[Li(thf)4][Ho(mbmp)2(thf)2] ⋅ 0.5 thf (14)

Synthesised as per 6 but with holmium filings (0.50 g, 3.00 mmol) in place of lanthanum to form 3 before treatment with nBuLi. Crystals grew overnight from the mother liquor (0.63 g, 63%). M. p. 182–184 °C; Anal. Calc. for C54H76O6HoLi (993.05 g.mol−1 after loss of four coordinated thf and half of a lattice thf): C 65.31, H 7.71, Ho 16.61. Found: C 64.87, H 7.44, Ho 16.15%. IR (Nujol, cm−1): 2725 m, 2586 w, 2365 w, 2275 m, 1907 m, 1732 s, 1601 s, 1556 m, 1204 w, 1143 w, 1074 m, 1029 s, 861 m, 792 m, 722 m, 673 s, 587 s.

[AlMe2Pr(mbmp)2(thf)2] ⋅ 2 C6D6 (15)

Synthesised as per 7 to form either [Pr(mbmp)(mbmpH)(thf)n] or [Pr2(mbmp)3(thf)x] then treated with AlMe3 (2.00 M, 0.5 mL, 1.00 mmol) in place of n‐BuLi. Crystals were grown overnight from C6D6 (0.32 g, 31%). M. p. 130–132 °C; Anal. Calc. for C56H82O6PrAl (1019.14 g.mol−1 after loss of two lattice C6D6): C 66.00, H 8.11, Pr 13.83. Found: C 59.48, H 7.82, Pr 13.51%. IR (Nujol, cm−1): 2381 s, 2271 s, 2083 w, 2034 m, 1895 m, 1752 s, 1703 s, 1609 s, 1376 w, 1250 m, 1102 m, 1021 s, 967 w, 865 m, 788 s, 718 m, 692 s.

[AlMe2Sm(mbmp)2(thf)2] ⋅ 2 C6D6 (16)

Synthesised as per 15 but with samarium filings (0.45 g, 3.00 mmol) in place of praseodymium to form 1 before treatment with AlMe3. Crystals grew overnight from C6D6 (0.45 g, 42%). Anal. Calc. for C59H82D3O6SmAl (1070.66 g.mol−1 after loss of one and a half lattice C6D6): 66.19, H 8.28, Sm 14.04. Found: C 66.04, H 8.13, Sm 13.82%. IR (Nujol, cm−1): 2381 s, 2271 s, 2083 w, 2034 m, 1895 m, 1752 s, 1703 s, 1609 s, 1376 w, 1250 m, 1102 m, 1021 s, 967 w, 865 m, 788 s, 718 m, 692 s.

[AlMe2Tb(mbmp)2(thf)2] ⋅ 2 C6D6 (17)

Synthesised as per 15 but with terbium filings (0.47 g, 3.00 mmol) in place of praseodymium to form 2 before treatment with AlMe3. Crystals grew overnight from C6D6 (0.53 g, 51%). M. p. 175–177 °C; Anal. Calc. for C56H82O6TbAl (1037.15 g.mol−1 after loss of two lattice C6D6): C 64.85, H 7.97, Tb 15.32. Found: C 64.57, H 7.63, Tb 15.08%. 1H‐NMR (400 MHz, C6D6, 25 °C): δ=7.28 (s, 4H, ArH), 7.18 (s, 4H, ArH), 4.23 (d, 2H, CH2), 3.59 (d, 2H, CH2 (masked by thf signal), 3.56 (m, 8H, OCH2, thf), 2.29 (s, 12H, CH3), 1.61 (s, 36H, C(CH3)3), 0.97 (s, 8H, CH2, thf), −0.27 (s, 6H, Al(CH3) ppm. IR (Nujol, cm−1): 2385 w, 2297 s, 1744 s, 1454 s, 1372 s, 1278 s, 1196 s, 1029 m, 996 s, 914 m, 895 s, 800 m.

[La(mbmp)(thf)4][AlMe2(mbmp)] ⋅ thf (18)

Synthesised as per 15 but with lanthanum filings (0.42 g, 3.00 mmol) in place of praseodymium to form either [La(mbmp)(mbmpH)(thf)n] or [La2(mbmp)3(thf)x] before treatment with AlMe3. Crystals grew overnight from the mother liquor (0.38 g, 35%). M. p. 180–182 °C; Anal. Calc. for C60H90O7LaAl (1089.24 g.mol−1 after loss of one lattice and two coordinated thf): C 66.16, H 8.33, La 12.75. Found: C 66.04, H 8.21, La 12.34%. IR (Nujol, cm−1): 2373 w, 2283 w, 2030 w, 1891 m, 1744 s, 1605 s, 1239 w, 1021 m, 865 m, 665 m.

[K(thf)3Gd(mbmp)2(thf)2] ⋅ 0.5 thf (19)

Synthesised as per 6 but with gadolinium filings (0.47 g, 3.00 mmol) in place of lanthanum to form [Gd(mbmp)(mbmpH)(thf)3], and KN(SiMe3)2 (0.50 M, 0.5 mL, 1.00 mmol) in place of n‐BuLi. Crystals grew overnight from the mother liquor (0.65 g, 53%). M. p. 268–270 °C; Anal. Calc. for C66H100O9GdK (1233.84 g.mol−1 after loss of half of a lattice thf): C 64.25, H 8.17, Gd 12.74. Found: C 63.79, H 7.82, Gd 12.36. IR (Nujol, cm−1): 2549 m, 2410 w, 2369 w, 2283 w, 2079 m, 1891 m, 1744 s, 1609 s, 1560 m, 1233 m, 959 w, 681 s, 583 m.

[ZnEtYb(mbmp)2(thf)] ⋅ 2 C6D6 (20)

Synthesised as per 6 but with ytterbium filings (0.52 g, 3.00 mmol) in place of lanthanum to form 4, and ZnEt2 (1.00 M, 1.00 mL, 1.00 mmol) was used in place of n‐BuLi. Crystals grew overnight from C6D6 (0.70 g, 66%). M. p. 138–140 °C; Anal. Calc. for C55H73D3O5YbZn (1058.64 g.mol−1 after loss of one and a half lattice C6D6): C 62.40, H 7.52. Found: C 62.18, H 7.37%. IR (Nujol, cm−1): 2553 w, 2434 w, 2377 m, 2267 s, 2132 m, 2034 m, 1748 s, 1605 s, 1376 w, 1208 m, 628 m.

Crystal and refinement data

Single crystals covered with viscous hydrocarbon oil were mounted on a glass fibre. Data were obtained at −173 °C (100 K) on the MX1: Macromolecular Crystallography beamline at the Australian Synchrotron, Victoria, Australia. Data collection and integration on the MX1: Macromolecular Crystallography beamline was accomplished using Blu‐Ice. [27] The structures were solved using SHELXS7 and refined by full‐matrix least‐squares on all F2 data using SHELX2014 [28] in conjunction with the X‐Seed graphical user interface. [29] All hydrogen atoms were placed in calculated positions using the riding model. Data collection and refinement details are collated in the SI (Table S1).

Conflict of interest

The authors declare no conflict of interest.

1.

Supporting information

As a service to our authors and readers, this journal provides supporting information supplied by the authors. Such materials are peer reviewed and may be re‐organized for online delivery, but are not copy‐edited or typeset. Technical support issues arising from supporting information (other than missing files) should be addressed to the authors.

Supporting Information

Acknowledgements

Open access publishing facolitated by James Cook University, as part of Wiley – James Cook University agreement via the Council of Australian University Librararians. This research was supported by Australian Research Council (DP190100798), Part of the research were undertaken on the MX1 beamline at the Australian Synchrotron, part of ANSTO. Open access publishing facilitated by James Cook University, as part of the Wiley ‐ James Cook University agreement via the Council of Australian University Librarians.

S. H. Ali, A. C. G. Shephard, J. Wang, Z. Guo, M. S. Davies, G. B. Deacon, P. C. Junk, Chem. Asian J. 2022, 17, e202101328.

Data Availability Statement

The data that support the findings of this study are available from the corresponding author upon reasonable request.

References

  • 1. Bradley D. C., Mehrotra R. C., Rothwell I. P., Singh A., Alkoxo and Aryloxo Derivatives of Metals, Academic Press, London, 2001. [Google Scholar]
  • 2. Boyle T. J., Ottley L. A. M., Chem. Rev. 2008, 108, 1896–1917. [DOI] [PubMed] [Google Scholar]
  • 3. Ortu F., Mills D. P., Handbook on the Physics and Chemistry of Rare Earths, Volume 55, Ch. 306, 2019. [Google Scholar]
  • 4. Aspinall H. C., Bickley J. F., Gaskell J. M., Jones A. C., Labat G., Chalker P. R., Williams P. A., Inorg. Chem. 2007, 46, 5852–5860. [DOI] [PubMed] [Google Scholar]
  • 5. Lyubov D. M., Tolpygin A. O., Trifonov A. A., Coord. Chem. Rev. 2019, 392, 83–145. [Google Scholar]
  • 6. Deng M., Yao Y., Shen Q., Zhang Y., Sun J., Dalton Trans. 2004, 944–950. [DOI] [PubMed] [Google Scholar]
  • 7. Qi R., Liu B., Xu X., Yang Z., Yao Y., Zhang Y., Shen Q., Dalton Trans. 2008, 5016–5024. [DOI] [PubMed] [Google Scholar]
  • 8. Liang Z., Ni X., Li X., Shen Z., Inorg. Chem. Commun. 2011, 14, 1948–1951. [Google Scholar]
  • 9. Tan Y.-F., Xu X.-P., Guo K., Yao Y.-M., Zhang Y., Shen Q., Polyhedron 2013, 61, 218–224. [Google Scholar]
  • 10. Bao L., Yingming Y., Mingyu D., Yong Z., Qi S., J. Rare Earth 2006, 24, 264–267. [Google Scholar]
  • 11. Xu B., Huang L., Yang Z., Yao Y., Zhang Y., Shen Q., Organometallics 2011, 30, 3588–3595. [Google Scholar]
  • 12. Deacon G. B., Forsyth C. M., Nickel S., J. Organomet. Chem. 2002, 647, 50–60. [Google Scholar]
  • 13. Guo Z., Huo R., Tan Y. Q., Blair V., Deacon G. B., Junk P. C., Coord. Chem. Rev. 2020, 415, 213232. [Google Scholar]
  • 14. Shephard A. C. G., Ali S. H., Wang J., Guo Z., Davies M. S., Deacon G. B., Junk P. C., Dalton Trans. 2021, 50, 14653. [DOI] [PubMed] [Google Scholar]
  • 15. Mahoney B. D., Piro N. A., Carroll P. J., Schelter E. J., Inorg. Chem. 2013, 52, 5970–5977. [DOI] [PubMed] [Google Scholar]
  • 16. Korobkov I., Gambarotta S., Organometallics 2009, 28, 4009. [Google Scholar]
  • 17.The survey was performed with CCDC: ConQuest 2020.3.0.
  • 18. Xu X., Zhang Z., Yao Y., Zhang Y., Shen Q., Inorg. Chem. 2007, 46, 9379–9388. [DOI] [PubMed] [Google Scholar]
  • 19. Thim R., Schädle D., Maichle-Mössmer C., Anwander R., Chem. Eur. J. 2019, 25, 507–511. [DOI] [PubMed] [Google Scholar]
  • 20. Deacon G. B., Delbridge E. E., Evans D. J., Harika R., Junk P. C., Skelton B. W., White A. H., Chem. Eur. J. 2004, 10, 1193–1204. [DOI] [PubMed] [Google Scholar]
  • 21. Yan K., Schoendorff G., Upton B. M., Ellern A., Windus T. L., Sadow A. D., Organometallics 2013, 32, 1300–1316. [Google Scholar]
  • 22. Buchanan W. D., Nagle E. D., Ruhlandt-Senge K., Main Group Chem. 2009, 8, 263–273. [Google Scholar]
  • 23. Chen X., Liu S., Du B., Meyers E. A., Shore S. G., Eur. J. Inorg. Chem. 2007, 5563–5570. [Google Scholar]
  • 24. Moore M., Gambarotta S., Bensimon C., Organometallics 1997, 16, 1086–1088. [Google Scholar]
  • 25. Deacon G. B., Cosgriff J. E., Lawrenz E. T., Forsyth C. M., Wilkinson D. L., in Herrmann-Brauer, Synthetic Methods of Organometallic and Inorganic Chemistry, ed. W. A. Herrmann, Thieme, Stuttgart, 1997, vol. 6, p.48. [Google Scholar]
  • 26. Lingane J. J., Complexometric Titrations., Methuen, London, 1958. [Google Scholar]
  • 27. McPhillips T. M., McPhillips S. E., Chiu H. J., Cohen A. E., Deacon A. M., Ellis P. J., Garman E., Gonzalez A., Sauter N. K., Phizackerley R. P., Soltis S. M., Kuhn P., J. Synchrotron Radiat. 2002, 9, 401–406. [DOI] [PubMed] [Google Scholar]
  • 28. Sheldrick G. M., Acta Crystallogr. Sect. C 2015, 71, 3–8. [DOI] [PMC free article] [PubMed] [Google Scholar]
  • 29. Barbour L. J., J. Supramol. Chem. 2001, 1, 189–191. [Google Scholar]

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Data Availability Statement

The data that support the findings of this study are available from the corresponding author upon reasonable request.


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