Martin J. D.
Champion
,
Paolo
Farina
,
William
Levason
* and
Gillian
Reid
School of Chemistry, University of Southampton, Southampton, SO17 1BJ, UK. E-mail: wxl@soton.ac.uk
First published on 9th July 2013
Complexes of the oxa-thia macrocycles [18]aneO4S2, [15]aneO3S2 and the oxa-selena macrocycle [18]aneO4Se2 (L) of types [MCl2(L)]FeCl4 (M = Sc or Y) were prepared from [ScCl3(thf)3] or [YCl2(THF)5][YCl4(THF)2] and the ligand in anhydrous MeCN, using FeCl3 as a chloride abstractor. The [MI2(L)]I, [LaI3(L)] and [LuI2(L)]I have been prepared from the ligands and the appropriate anhydrous metal triiodide in MeCN. Complexes of type [LaI3(crown)] and [LuI2(crown)]I (crown = 18-crown-6, 15-crown-5) were made for comparison. Use of the metal iodide results in complexes with high solubility compared to the corresponding chlorides, although also with increased sensitivity to moisture. All complexes were characterised by microanalysis, IR, 1H, 45Sc and 77Se NMR spectroscopy as appropriate. X-ray crystal structures are reported for [ScCl2([18]aneO4S2)][FeCl4], [ScI2([18]aneO4S2)]I, [YCl2(18-crown-6)]3[Y2Cl9], [YCl2([18]aneO4S2)][FeCl4], [LaI3(15-crown-5)], [LaI2(18-crown-6)(MeCN)]I, [LuI(18-crown-6)(MeCN)2]I2, [Lu(15-crown-5)(MeCN)2(OH2)]I3, [LaI3([18]aneO4S2)], [LaI([18]aneO4S2)(OH2)]I2, [LaI3([18]aneO4Se2)] and [LuI2([18]aneO4Se2)]I. In each complex all the neutral donor atoms of the macrocycles are coordinated to the metal centre, showing very rare examples of these oxophilic metal centres coordinated to thioether groups, and the first examples of coordinated selenoether donors. In some cases MeCN or adventitious water displaces halide ligands, but not the S/Se donors from La or Lu complexes. A complex of the oxa-tellura macrocycle [18]aneO4Te2, [ScCl2([18]aneO4Te2)][FeCl4] was isolated, but is unstable in MeCN solution, depositing elemental Te. YCl3 and 18-crown-6 produced [YCl2(18-crown-6)]3[Y2Cl9], the asymmetric unit of which contains two cations with a trans-YCl2 arrangement and a third with a cis-YCl2 group.
In this work, anhydrous lanthanide iodides were generally used in preference to the corresponding chlorides due to their higher solubility in weakly coordinating solvents like MeCN, which mainly reflects the lower lattice energies of MI3 compared to the lighter halides. In the scandium and yttrium systems, cationic chloride species generated using FeCl3 as a chloride abstractor were also prepared.
IR spectra were obtained as Nujol mulls on a Perkin Elmer Spectrum 100 spectrometer. 1H and 19F{1H} NMR spectra were recorded on a Bruker AV 300 spectrometer and referenced to residual solvent (1H) and external CFCl3 (19F). 77Se{1H} NMR spectra were obtained on a Bruker DPX400 and referenced to neat external Me2Se. 45Sc, 89Y and 139La NMR spectra were recorded on a Bruker DPX400 and are referenced to external aqueous solutions of the corresponding aquo-cations at pH = 1 in water. Microanalysis were conducted by Medac Ltd or London Metropolitan University. Conductivity measurements were carried out under inert atmosphere, using a platinum electrode conductivity cell on a PYE & Co conductance bridge.
For [LaI([18]aneO4S2)(OH2)]I2·H2O the crystal quality was modest and H-atoms on the water oxygens were not found. [LaI3([18]aneO4S2)] – Disorder was evident in the crown backbone at C(3) and C(4), which was satisfactorily modelled as two sites C3A,C3B and C4A,C4B, with refined occupancies of 60%:
40%. In [LaI3(15-crown-5)]·MeCN the molecule has mirror symmetry and carbon atoms C1, C4 and C5 are disordered over two sites (A/B) which was satisfactorily modelled. [Lu(MeCN)2(18-crown-6)I]I2 – The crystal quality was rather poor with large Q peaks near to Lu and I, hence while the structure confirms the connectivities, detailed comparisons of bond distances etc. should be treated with caution. In [LuI2([18]aneO4Se2)]I·2MeCN disorder at C2 and C5 was modelled as two sites (A/B) and it was necessary to ‘split’ C1 and C6, which were refined as C1/C1B and C6/C6B (both pairs with the same coordinates and same Uij) to add H atoms. Some slight disorder of the carbon backbone was apparent in the structure of [ScI2([18]aneO4S2)]I·MeCN, and two C atoms were modelled as disorder over two sites.
CCDC reference numbers 940218–940229 contain crystallographic data in cif format.
The 15-membered ring thia-oxa macrocycle [15]aneO3S2 ([15]aneO3S2 = 1,4-dithia-7,10,13-trioxacyclopentadecane) reacted with [ScCl3(THF)3] in the presence of one molar equivalent of FeCl3 to form [ScCl2([15]aneO3S2)][FeCl4], and with anhydrous ScI3 to form yellow [ScI2([15]aneO3S2)]I. Attempts to use SbCl5 as a chloride abstractor for the thia-oxa macrocycle complexes resulted in intensely coloured solutions due to redox chemistry at sulfur leading to Sb(III) complexes,17 and even FeCl3 cannot be used in the iodide systems due to instability of FeI3.27 The complexes are extremely sensitive to moisture and attempts to obtain crystals suitable for an X-ray study have been unsuccessful. The IR spectrum of [ScCl2([15]aneO3S2)][FeCl4] confirms the absence of MeCN and shows strong bands at 380 cm−1 assigned to [FeCl4]−28 and 363 and 293 cm−1ν(ScCl). The 1H NMR spectra of both complexes in CD3CN show broad resonances with no resolved couplings to high frequency of those in [15]aneO3S2, whilst they show broad singlets in the 45Sc NMR spectra (Table 1).§ The high frequency 45Sc chemical shifts (compared to the 15-crown-5 complex) are consistent with coordination of the sulfur in the [15]aneO3S2 complexes. The high frequency shift I > Cl is also consistent with data on scandium halide-phosphine oxide systems.29
Complex | δ(45Sc) | Ref. |
---|---|---|
a 295 K in MeCN solution. n.o. not observed. | ||
[ScCl2([15]aneO3S2)][FeCl4] | 201 | This work |
[ScI2([15]aneO3S2)]I | 297 | This work |
[ScCl2(15-crown-5)][FeCl4] | 130 | 3, 4 |
[ScCl(MeCN)(15-crown-5)][FeCl4]2 | 99.5 | 3 |
[ScCl2([18]aneO4S2)][FeCl4] | 202 | This work |
[ScCl2([18]aneO4Se2)][FeCl4] | 205 | This work |
[ScCl2(18-crown-6)][FeCl4] | 132 | 3 |
[ScI2([18]aneO4S2)]I | See text | This work |
[ScI2([18]aneO4Se2)]I | n.o. | This work |
The reaction of [ScCl3(THF)3] with the 18-membered ring thia-oxa macrocycle, [18]aneO4S2 in the presence of FeCl3 produced yellow [ScCl2([18]aneO4S2)][FeCl4], for which yellow crystals were grown from MeCN–CH2Cl2 solution. The structure (Fig. 1) shows the scandium cation coordinated to all six donors of the ring and two cis disposed chlorines (Cl–Sc–Cl 97.7(1)°). The structure contrasts with those of [ScCl2(18-crown-6)]Y3,4 which have a trans arrangement of the chlorides and with only five of the six available oxygen donor atoms coordinated to the scandium. The Sc–O distances in the present complex, 2.247(8)–2.435(8) Å, are more disparate than in [ScCl2(18-crown-6)][FeCl4] (2.195(2)–2.264(2) Å). We note that in exo-coordinated crown and thia-oxacrown complexes of CrCl3 and VCl3, coordination of sequential donor groups produced very acute O–M–O angles, whereas the S–M–S angles did not show similar effects, due to the longer M–S bonds,30 and this resulted in preferential sulfur coordination to the hard metal centres. In the present case, the longer Sc–S bonds of 2.74 Å (av) allows the ring to coordinate all six donors to the small scandium centre, with some small amount of folding of the macrocycle. In CD3CN or d6-acetone solutions the 1H NMR spectra contain several broad resonances shifted to high frequency from those in the ligand; these sharpen on cooling the solutions, but even at low temperatures they remain broad, indicative of dynamic processes. The 45Sc NMR resonance, δ = 204, is similar to that in the [15]aneO3S2 complex, but some 70 ppm to high frequency of the 18-crown-6 complex (Table 1). The reaction of ScI3 with [18]aneO4S2 in rigorously anhydrous MeCN produced deep yellow [ScI2([18]aneO4S2)]I, the structure of which (Fig. 2) reveals a very similar geometry to the chloride. The 45Sc NMR resonance observed at δ = 206, seems inconsistent with the presence of coordinated iodide, and it may be that the iodides are displaced in solution by MeCN which would produce a significant low frequency shift.
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Fig. 1 The structure of the Sc1 centred cation in [ScCl2([18]aneO4S2)][FeCl4] showing the atom labelling scheme. The other two independent scandium cations are similar. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): Sc1–O1 = 2.247(8), Sc1–O3 = 2.256(8), Sc1–O4 = 2.390(8), Sc1–O2 = 2.435(8), Sc1–S2 = 2.734(3), Sc1–S1 = 2.753(3), Sc1–Cl1 = 2.422(3), Sc1–Cl2 = 2.466(3), O1–Sc1–O2 = 67.9(3), O3–Sc1–O4 = 70.6(3), O3–Sc1–S2 = 70.3(2), O2–Sc1–S2 = 69.29(19), O4–Sc1–S1 = 69.16(19), O1–Sc1–S1 = 74.5(2), Cl2–Sc1–S1 = 79.36(10), Cl1–Sc1–Cl2 = 97.67(11), S2–Sc1–S1 = 139.97(11). |
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Fig. 2 The structure of the cation in [ScI2([18]aneO4S2)]I·MeCN showing the atom labelling scheme. The displacement ellipsoids are drawn at the 40% probability level and H atoms are omitted for clarity. The cation has mirror symmetry. C2 and C5 were modelled as two disordered sites and only the major A site is shown. Symmetry operation: i = x, 1/2 − y, z. Selected bond lengths (Å) and angles (°): Sc1–O1 = 2.272(8), Sc1–O2 = 2.263(9), Sc1–S1 = 2.711(5), Sc1–S2 = 2.715(4), Sc1–I1 = 2.915(2), O1–Sc1–O2 = 69.0(3), O1–Sc1–S1 = 71.8(2), O2–Sc1–S2 = 70.7(2), O1–Sc1–I1 = 86.9(3), O2–Sc1–I1 = 86.3(3), S1–Sc1–I1 = 75.17(8), S2–Sc1–I1 = 76.00(8), I1–Sc1–I1 = 94.03(9), S1–Sc1–S2 = 137.16(15). |
Replacing [18]aneO4S2 with the selenium analogue [18]aneO4Se2 gave extremely moisture sensitive brownish yellow complexes [ScCl2([18]aneO4Se2)][FeCl4] and [ScI2([18]aneO4Se2)]I. Spectroscopically these two complexes, which constitute the first examples with Sc–Se coordination in a neutral ligand, closely resembled the thia-oxa analogues. We were unable to observe 45Sc or 77Se{1H} resonances from the iodo-complex, presumably due to exchange, but for [ScCl2([18]aneO4Se2)][FeCl4], the 45Sc chemical shift of 205, and a 77Se{1H} shift of +150 ppm compared to the ligand shift22 of +140 ppm, are evidence of the Sc–Se interaction is maintained in solution.
The reaction of [18]aneO4Te2 with [ScCl3(THF)3] and FeCl3 in anhydrous MeCN gave a brown precipitated solid with a composition corresponding to [ScCl2([18]aneO4Te2)][FeCl4]. The IR spectrum, which showed the presence of the ligand and the absence of MeCN or THF, with [FeCl4]− at 378 cm−1 and a broad feature at ∼324 cm−1 assigned to ν(ScCl), support the formulation. A solution in CD3CN at ambient temperature rapidly darkens and deposits black tellurium, but from a solution made at 240 K and run immediately it was possible to obtain the 1H NMR spectrum, which showed very broad features of the tellura-oxa macrocycle. On standing in solution, new resonances appeared including a doublet at ∼5.5 ppm which may suggest a vinyl unit, along with a black precipitate. The 45Sc spectrum of a solution of the complex at 240 K contained several broad resonances, the relative intensities of which changed over time, and no useful conclusions could be drawn. This ligand contains quite reactive Te–C bonds in –Te(CH2)2– units which have a tendency to decompose with elimination of ethene,31 and it has limited coordination chemistry. It gives stable complexes bound as a Te2 donor in planar [MCl2([18]aneO4Te2)] (M = Pd or Pt),22 but decomposes rapidly on reaction with SbX316 or Pb(BF4)2
17 with precipitation of tellurium, and does not react with (or decompose with) MI2 (M = Ca or Sr) in MeCN.19 The scandium system seems to be a borderline case, in that a complex precipitates from the concentrated synthesis solution, but decomposes quite rapidly in dilute solution at ambient temperatures.
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Fig. 3 The structure of the Y3 centred cation in [YCl2(18-crown-6)]3[Y2Cl9]·nMeCN (n = 1.65) showing the atom labelling scheme. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): Y3–O14 = 2.413(4), Y3–O17 = 2.419(4), Y3–O13 = 2.426(3), Y3–O16 = 2.431(3), Y3–O18 = 2.448(4), Y3–O15 = 2.451(4), Y3–Cl5 = 2.5708(15), Y3–Cl6 = 2.5834(15), O14–Y3–O13 = 66.78(13), O17–Y3–O16 = 66.44(12), O17–Y3–O18 = 63.22(13), O13–Y3–O18 = 64.90(13), O14–Y3–O15 = 64.09(13), O16–Y3–O15 = 64.63(13), Cl5–Y3–Cl6 = 89.54(5). |
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Fig. 4 The structure of the Y1 centred cation in [YCl2(18-crown-6)]3[Y2Cl9]·nMeCN (n = 1.65) showing the atom labelling scheme. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): Y1–O6 = 2.409(4), Y1–O5 = 2.426(4), Y1–O1 = 2.438(4), Y1–O4 = 2.438(4), Y1–O2 = 2.460(5), Y1–O3 = 2.474(4), Y1–Cl1 = 2.5988(15), Y1–Cl2 = 2.6103(15), O6–Y1–O5 = 65.40(14), O6–Y1–O1 = 65.00(15), O5–Y1–O4 = 63.29(14), O1–Y1–O2 = 65.44(16), O4–Y1–O3 = 63.23(14), O2–Y1–O3 = 62.58(14), Cl1–Y1–Cl2 = 157.91(5). |
The reaction of [YCl2(THF)5][YcCl4(THF)2] (from YCl3 and THF)21 with FeCl3 and [18]aneO4S2, gave pale yellow [YCl2([18]aneO4S2)][FeCl4]. Crystals grown from MeCN solution by slow evaporation of the solvent showed a cis-dichloro arrangement with a Cl–Y–Cl angle of 94.6° (Fig. 5).
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Fig. 5 The structure of the cation in [YCl2([18]aneO4S2)][FeCl4] showing the atom labelling scheme. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): Y1–O2 = 2.3652(17), Y1–O4 = 2.4012(17), Y1–O3 = 2.4703(17), Y1–O1 = 2.4911(18), Y1–Cl1 = 2.5682(8), Y1–Cl2 = 2.5914(7), Y1–S2 = 2.8955(8), Y1–S1 = 2.9162(8), O4–Y1–O = 3 67.15(6), O2–Y1–O1 = 66.43(6), Cl1–Y1–Cl2 = 94.63(2), O2–Y1–S2 = 68.09(4), O3–Y1–S2 = 68.26(4), O4–Y1–S1 = 69.20(5), O1–Y1–S1 = 66.58(4). |
The [YCl2([15]aneO3S2)][FeCl4] was obtained similarly, and is assumed to contain a seven coordinate cation. More unusual are [YCl2([18]aneO4Se2)][FeCl4] and [YI2([18]aneO4Se2)]I, which contain the first examples of a neutral selenoether function coordinated to yttrium(III). The 1H NMR spectra of all the yttrium complexes of thia-oxa and selena-oxa macrocycles show broad resonances without resolved couplings consistent with dynamic behaviour in solution, and as for the 18-crown-6 complex we were unable to observe 89Y NMR spectra. However, for both of the selena-oxa-crown complexes, 77Se{1H} NMR resonances were observed with modest low frequency coordination shifts – for [YCl2([15]aneO3S2)][FeCl4] δ(77Se) = 103 and for [YI2([18]aneO4Se2)]I δ(77Se) = 125, compared to the ligand value of 140 ppm. If some [18]aneO4Se2 was added, the 77Se shifts of both complex and “free” ligand were unchanged, showing the ligand exchange is low on the NMR timescale. The broadening in the 1H NMR spectra must be due to processes other than complete dissociation of the macrocycle even in the d0 complexes; possibilities include reversible dissociation of single donors or inversion. In late d-block metal complexes selenoethers (including [18]aneO4Se2) usually exhibit high frequency coordination shifts, but with p-block metals and some early transition metals the coordination shifts are erratic, both high and low frequency shifts being observed in different systems.12,33
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Fig. 6 Structure of [LaI3(15-crown-5)]·MeCN showing the atom labelling scheme. Ellipsoids are drawn at the 50% probability level, and H atoms have been omitted for clarity. The molecule has mirror symmetry and carbon atoms C1, C4 and C5 are disordered over two sites (A/B) – both components are shown. Symmetry operation: i = x, 1/2 − y, z. Selected bond lengths (Å) and angles (°): La1–O3i = 2.587(5), La1–O3 = 2.587(5), La1–O2i = 2.590(5), La1–O2 = 2.590(5), La1–O1 = 2.626(7), La1–I2i = 3.1843(9), La1–I2 = 3.1843(9), La1–I1 = 3.2537(11), O3–La1–O3i = 62.7(2), O3–La1–O2 = 62.27(15), O2–La1–O1 = 61.41(14), I2–La1–I2i = 95.17(3), I2–La1–I1 = 80.72(2). |
The [LaI3(18-crown-6)] was isolated by reaction of LaI3 and the crown in CH2Cl2, but crystals grown from an MeCN solution were found to be [LaI2(18-crown-6)(MeCN)]I·nMeCN (Fig. 7) again showing the ease with which the iodide is displaced. The Ce and Nd analogues [MI3(18-crown-6)] were also isolated, along with crystals of the isomorphous complex [CeI2(18-crown-6)(MeCN)]I·0.5MeCN and are described in the ESI.† If the reaction of LaI3 and 18-crown-6 is conducted in MeCN solution in the presence of [NH4]PF6, the product is [LaI2(18-crown-6)]PF6. Lanthanum easily switches between eight- and nine-coordination depending upon the ligand set and the conditions. We also carried out conductivity measurements of several [MI3(crown)] complexes in 10−3 mol dm−3 MeCN and found the values (Experimental section) were much higher than expected for 1:
1 electrolytes, showing that in the very dilute solutions, the iodide ligands are displaced.34 In contrast, [La(O3SCF3)2(18-crown-6)][O3SCF3], prepared from La(O3SCF3)3 and the crown in MeCN (see ESI†), is a 1
:
1 electrolyte, showing that the hard triflate ligands are not easily displaced, contrasting with the soft iodide. All attempts to observe 139La NMR¶ spectra from iodide complexes failed, attributed to fast quadrupolar relaxation in the low symmetry environments. However, for [La(O3SCF3)2(18-crown-6)]+ in which the O8 donor set would be expected to produce a smaller electric field gradient, a broad resonance was observed at δ = −112 (W1/2 = 3000 Hz).
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Fig. 7 One of the two crystallographically distinct cations (La1 centred) in [LaI2(18-crown-6)(MeCN)]I·nMeCN showing the atom labelling scheme. Ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. La1–O are shown as open bonds. Selected bond lengths (Å) and angles (°): La1–O5 = 2.569(3), La1–O1 = 2.597(2), La1–O2 = 2.604(3), La1–O4 = 2.605(2), La1–O6 = 2.615(3), La1–N1 = 2.618(4), La1–O3 = 2.639(3), La1–I1 = 3.2152(5), La1–I2 = 3.2304(4), O1–La1–O2 = 62.22(8), O5–La1–O4 = 62.59(8), O5–La1–O6 = 60.83(8), O1–La1–O6 = 62.19(8), O2–La1–O3 = 60.64(8), O4–La1–O3 = 61.24(8), N1–La1–I1 = 140.82(8), N1–La1–I2 = 70.67(8), I1–La1–I2 = 147.857(12). |
Lutetium is significantly smaller than lanthanum and hence might be expected to favour a lower coordination number and/or smaller ligands. The complexes [LuI2(15-crown-5)]I and [LuI(18-crown-6)(MeCN)2]I2 were isolated from MeCN solutions of the constituents. Crystals of the latter showed (Fig. 8) the two nitrile ligands arranged on one side and the iodide on the other side of the puckered macrocycle ring. Comparisons of the bond lengths from the structures in Fig. 7 and 8 clearly show the effect of the decreased radius of Lu3+.
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Fig. 8 The structure of the cation in [LuI (18-crown-6)(MeCN)2]I2 showing the atom labelling scheme. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. The cation has mirror symmetry. Symmetry operation: a = x, 1/2 − y, z. Selected bond lengths (Å) and angles (°): Lu1–O1 = 2.353(13), Lu1–O2 = 2.405(9), Lu1–O3 = 2.423(8), Lu1–N1 = 2.425(11), Lu1–O4 = 2.432(11), Lu1–I1 = 3.075(2), O1–Lu1–O2 = 64.8(2), O2–Lu1–O3 = 64.5(3), N1–Lu1–N1a = 71.7(5), O3–Lu1–O4 = 66.0(3), N1–Lu1–I1 = 143.1(2). |
Crystals grown from an MeCN solution of [LuI2(15-crown-5)]I were found to be [Lu(15-crown-5)(MeCN)2(OH2)]I3, where all three iodides had been displaced by MeCN and adventitious water (Fig. 9).
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Fig. 9 The structure of the cation in [Lu(15-crown-5)(MeCN)2(OH2)]I3 showing the atom labelling scheme. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. The cation has mirror symmetry. Symmetry operation: a = x, 1/2 − y, z. Selected bond lengths (Å) and angles (°): Lu1–O4 = 2.257(5), Lu1–O3 = 2.303(4), Lu1–O1 = 2.317(5), Lu1–O2 = 2.361(3), Lu1–N1 = 2.401(4), O3–Lu1–O3a = 65.30(18), O3–Lu1–O2 = 67.09(13), O1–Lu1–O2 = 67.78(9), N1–Lu1–N1a = 70.3(2). |
The complexes [LaI3([15]aneO3S2)], [LaI3([18]aneO4S2)], [LaI3([18]aneO4Se2)], [NdI3([18]aneO4Se2)], [LuI2([18]aneO4S2)]I and [LuI2([18]aneO4Se2)]I were isolated from reaction of the appropriate lanthanide iodide with the ligands in anhydrous MeCN. The spectroscopic data and microanalyses are consistent with the formulations, but the main interest lies in the structures. The [LaI3([18]aneO4S2)] and [LaI3([18]aneO4Se2)] are isomorphous and contain nine-coordinate lanthanum centres with the metal endo-coordinated to all six donors of the puckered ring and with two iodides above and one below the plane (Fig. 10 and 11). The La–O and La–I bond distances are not significantly different between the two structures, but interestingly the La–S and La–Se differ only by ∼0.01 Å, compared to the differences in covalent radii of the chalcogens of 0.015 Å.35 Whilst this could be seen as evidence of stronger interaction with the selenium donors, this seems unlikely and a possible explanation is that the constraints of the macrocycle ring play a significant role in the M–S/Se bond lengths. The structure was also obtained of the hydrolysis product [LaI([18]aneO4S2)(OH2)]I2·H2O (Fig. 12).
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Fig. 10 Structure of [LaI3([18]aneO4S2)] showing the atom labelling scheme. Ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. C3 and C4 were disordered and modelled as two sites A/B. Only the 3A and 4A sites are shown in the figure. Selected bond lengths (Å) and angles (°): La1–O3 = 2.582(4), La1–O2 = 2.618(4), La1–O4 = 2.622(4), La1–O1 = 2.635(4), La1–S2 = 3.004(1), La1–S1 = 3.015(2), La1–I2 = 3.2678(6), La1–I3 = 3.2999(7), La1–I1 = 3.3124(6), O3–La1–O4 = 63.74(12), O2–La1–O1 = 63.1(2), O4–La1–S2 = 66.23(9), O1–La1–S2 = 65.20(10), O3–La1–S1 = 64.68(9), O2–La1–S1 = 66.26(11), S2–La1–S1 = 144.76(4), I2–La1–I3 = 77.877(13), I2–La1–I1 = 141.33(2), I3–La1–I1 = 140.735(14). |
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Fig. 11 Structure of [LaI3([18]aneO4Se2)] showing the atom labelling scheme. Ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): La1–O1 = 2.560(3), La1–O2 = 2.604(3), La1–O4 = 2.609(4), La1–O3 = 2.634(3), La1–Se2 = 3.0885(7), La1–Se1 = 3.0971(7), La1–I2 = 3.2658(6), La1–I3 = 3.3244(7), La1–I1 = 3.3565(6), O1–La1–O2 = 64.27(10), O4–La1–O3 = 63.88(11), O2–La1–Se2 = 67.96(7), O3–La1–Se2 = 66.56(8), O1–La1–Se1 = 64.51(7), O4–La1–Se1 = 67.62(8), Se2–La1–Se1 = 140.63(2), I2–La1–I3 = 78.705(11), I2–La1–I1 = 141.297(14), I3–La1–I1 = 139.502(13). |
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Fig. 12 Structure of the cation in [LaI ([18]aneO4S2)(OH2)2]I2·H2O showing the atom labelling scheme. Ellipsoids are drawn at the 50% probability level and H atoms on C are omitted for clarity. H atoms were not identified on the water ligands. Selected bond lengths (Å) and angles (°): La1–O5 = 2.508(5), La1–O6 = 2.519(5), La1–O3 = 2.568(5), La1–O2 = 2.588(5), La1–O1 = 2.606(5), La1–O4 = 2.608(6), La1–S2 = 3.012(2), La1–S1 = 3.063(2), La1–I1 = 3.2385(7), O5–La1–O6 = 136.3(2), O3–La1–O2 = 104.60(15), O2–La1–O1 = 64.18(15), O3–La1–O4 = 62.92(15), O1–La1–S2 = 65.15(11), O4–La1–S2 = 66.27(12), O3–La1–S1 = 64.67(11), O2–La1–S1 = 64.34(11), S2–La1–S1 = 147.69(5), O5–La1–I1 = 147.54(13), O6–La1–I1 = 76.13(12). |
The lutetium complexes [LuI2([18]aneO4S2)]I and [LuI2([18]aneO4Se2)]I are isomorphous|| and contain eight-coordinate metal centres, reflecting the decreasing metal radius compared to lanthanum. The structure of [LuI2([18]aneO4Se2)]I shows the macrocycle ring is more folded and both iodides are on the same side of the metal, but compared to the geometry in [LaI3([18]aneO4Se2)], the differences in bond lengths are much as expected given the reduced metal radius of Lu3+.
The 1H NMR spectra of this series of compounds show broad singlets for the inequivalent methylene groups, but again couplings are not resolved. For the [LaI3([18]aneO4Se2)] and [LuI2([18]aneO4Se2)]I the 77Se{1H} spectra show small low frequency coordination shifts of −3 (La) and −32 (Lu), and in the presence of free [18]aneO4Se2 the chemical shifts are unchanged, showing exchange of the macrocycle is slow on the NMR timescale (Fig. 13).
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Fig. 13 The structure of the cation in [LuI2([18]aneO4Se2)]I·2MeCN showing the atom labelling scheme. The displacement ellipsoids are drawn at the 50% probability level and H atoms are omitted for clarity. The cation has mirror symmetry. Symmetry operation: i = x, 1/2 − y, z. Selected bond lengths (Å) and angles (°): Lu1–O2 = 2.348(8), Lu1–O1 = 2.368(8), Lu1–Se2 = 2.8959(18), Lu1–Se1 = 2.9034(17), Lu1–I1 = 2.9974(10), O2–Lu1–O1 = 68.1(3), O2–Lu1–Se2 = 69.8(2), O1–Lu1–Se1 = 71.32(18), Se2–Lu1–Se1 = 139.19(5), I1–Lu1–I1i = 94.67(4). |
The 1H NMR spectra of the complexes in solution at ambient temperatures show resonances broadened to varying degrees and without resolved couplings, indicative of dynamic processes. However, use of 77Se NMR spectroscopy to study the selena-oxa crown complexes both with and without added macrocycle, show that ligand exchange between coordinated and ‘free’ macrocycle is slow on the NMR timescale, hence the dynamic processes seen in the 1H NMR spectra would seem to be due to reversible dissociation of single donor centres, rather than intermolecular ligand exchange. The stability of the thia-oxa and selena-oxa macrocyclic complexes raises the prospect that complexes of macrocycles with higher chalcogen content, or even of homoleptic large thia- or selena-crowns, may be obtainable under appropriate anhydrous conditions and using the MI3 or MCl3 + chloride abstractor synthon strategy, and this will form the basis of a further study.
Footnotes |
† Electronic supplementary information (ESI) available: A table of crystallographic parameters. Synthesis and spectroscopic data for the (18-crown-6) and 15-crown-5 halide complexes of La, Lu, Ce or Nd discussed in the main text and for [La(O3SCF3)2(18-crown-6)][O3SCF3]. Figure and selected bond length and angle data for the cation in [CeI2(18-crown-6)(MeCN)]I·nMeCN, and for [Y3Cl9]3− anion in [YCl2(18-crown-6)]3[Y2Cl9]. CCDC 940218–940229. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c3dt51405f |
‡ “Lanthanide” also includes Y and Sc in this general discussion. |
§ 45Sc has I = 7/2, 100%, Ξ = 29.24 MHz, Q = −0.22 × 10−28 m2, Rc = 1710. |
¶ 139La I = 7/2, 99.9%, Ξ = 14.13 MHz, Q = −0.21 × 10−28 m2, Rc = 336. |
|| Poor quality crystals of [LuI2([18]aneO4S2)]I·2MeCN were isomorphous with the selena-oxo-crown analogue. a = 15.440(6), b = 11.847(4), c = 14.821(6), α = β = γ = 90, V = 2711.2(18), z = 4. The crystal quality was poor and refined to give R1 (I > 2σI) = 0.0986. |
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