DOI:
10.1039/C5DT03941J
(Paper)
Dalton Trans., 2015,
44, 20898-20905
Cationic aza-macrocyclic complexes of germanium(II) and silicon(IV)†
Received
8th October 2015
, Accepted 6th November 2015
First published on 9th November 2015
Abstract
[GeCl2(dioxane)] reacts with the neutral aza-macrocyclic ligands L, L = Me3tacn (1,4,7-trimethyl-1,4,7-triazacyclononane), Me4cyclen (1,4,7,10-tetramethyl-1,4,7,10-tetraazacyclododecane) or Me4cyclam (1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane) and two mol. equiv. of Me3SiO3SCF3 in thf solution to yield the unusual and hydrolytically very sensitive [Ge(L)][O3SCF3]2 as white solids in moderate yield. Using shorter reaction times [Ge(Me3tacn)]Cl2 and [Ge(Me3tacn)]Cl[O3SCF3] were also isolated; the preparation of [Ge(Me4cyclen)][GeCl3]2 is also described. The structures of the Me3tacn complexes show κ3-coordination of the macrocycle, with the anions interacting only weakly to produce very distorted five- or six-coordination at germanium. In contrast, the structure of [Ge(Me4cyclen)][O3SCF3]2 shows no anion interactions, and a distorted square planar geometry at germanium from coordination to the tetra-aza macrocycle. Crystal structures of the Si(IV) complexes, [SiCl3(Me3tacn)]Y (Y = O3SCF3, BArF; [B{3,5-(CF3)2C6H3}4]) and [SiHCl2(Me3tacn)][BArF], obtained from reaction of SiCl4 or SiHCl3 with Me3tacn, followed by addition of either Me3SiO3SCF3 or Na[BArF], contain distorted octahedral cations, with facial κ3-coordinated Me3tacn. The open-chain triamine, Me2NCH2CH2N(Me)CH2CH2NMe2 (pmdta), forms [SiCl3(pmdta)][BArF] and [SiBr3(pmdta)][BArF] under similar conditions, containing mer-octahedral cations.
Introduction
Elemental silicon and germanium and their compounds with oxygen and chalcogens are key technological materials, with applications in electronics, glasses, ceramics and optics.1–3 We are currently developing routes to electrochemically deposit the elements and their binary and ternary alloys from both organic solvents and supercritical fluids.4–6 In the search for silicon and germanium reagents with appropriate chemical stabilities and solubilities in these media for electrochemical studies, we have explored a variety of coordination complexes, to establish how the properties may be tuned by incorporating various ligands. Most coordination chemistry of germanium(II), germanium(IV) and silicon(IV) involves neutral adducts of the di- or tetra-halides,7 and cationic complexes are rather rare, while Si(II) halide complexes are limited to N-heterocyclic carbenes.8 Aza-macrocyclic complexes reported include [GeF3(Me3tacn)]2[GeF6] (Me3tacn = 1,4,7-trimethyl-1,4,7-triazacyclononane),9 [(GeF4)2(κ2κ′2-Me4cyclam)] (Me4cyclam = 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane),9 [GeCl3(Me3tacn)]2(H3O)2Cl3,10 [SiF3(Me3tacn)][SiF5],11 [Ge(Me3tacn)]Br[GeBr3],12 and [Ge(Me4cyclam)][GeCl3]2.12
Here we report the synthesis of several new Ge(II) mono- and dications and Si(IV) monocations based upon neutral triaza- and tetra-aza macrocyclic ligands with a variety of anions. Single crystal X-ray structural studies on representative examples are described and compared.
Experimental
SiCl4, SiHCl3, Me3SiO3SCF3, [GeCl2(dioxane)] and the N-donor ligands were obtained from Sigma Aldrich, except for Me3tacn which was prepared using the literature route.13 Na[BArF] ([BArF]− = [B{3,5-(CF3)2C6H3}4]−) was synthesised by a modification of Brookhart's procedure.14 Me2NCH2CH2N(Me)CH2CH2NMe2 (pmdta) was distilled from CaH2. All experiments were performed under strictly anhydrous conditions using glove-boxes and Schlenk techniques. CH2Cl2 was dried by distillation from CaH2, toluene was distilled from sodium, hexane was distilled from Na/K alloy and thf was distilled from Na/benzophenone ketyl. IR spectra were recorded as Nujol mulls between CsI plates using a Perkin Elmer Spectrum 100 spectrometer over the range 4000–200 cm−1. 1H and 19F NMR spectra were recorded using a Bruker DPX-400 spectrometer and referenced to the residual solvent resonance and external CFCl3, respectively. Microanalytical measurements were performed by London Metropolitan University.
[Ge(Me4cyclen)][O3SCF3]2
[GeCl2(dioxane)] (0.059 g, 0.26 mmol) was dissolved in thf (10 mL) and a solution of Me3SiO3SCF3 (0.112 g, 0.50 mmol) in thf (5 mL) was added with stirring, giving a clear, colourless solution. After 10 min, a solution of Me4cyclen (0.057 g, 0.25 mmol) in thf (5 mL) was added, causing the formation of a white precipitate. After stirring for a further 1 h, the product was collected by filtration and dried in vacuo. Yield: 0.120 g (80%). Anal. calc. for C14H28F6GeN4O6S2 (599.1): C, 28.08; H, 4.71; N, 9.35. Found: C, 28.19; H, 4.61; N, 9.26%. 1H NMR (CD3CN, 298 K): 2.78 (s, [12H], NCH3), 3.20–3.40 (m, [16H], NCH2). 19F{1H} NMR (CD3CN, 298 K): −79.4 (O3SCF3). IR (Nujol/cm−1): 474w, 517m, 573m, 638s, 749m, 793w, 919w, 960w, 1030s, 1068w, 1155s, 1225s, 1260s.
Crystals of [Ge(Me4cyclen)][O3SCF3]2·CH3CN suitable for X-ray diffraction were obtained by layering an acetonitrile solution with diethyl ether.
[Ge(Me4cyclam)][O3SCF3]2
[GeCl2(dioxane)] (0.058 g, 0.25 mmol) was dissolved in thf (10 mL), and a solution of Me3SiO3SCF3 (0.115 g, 0.52 mmol) in thf (5 mL) was added with stirring, giving a colourless solution. After 10 min a solution of Me4cyclam (0.065 g, 0.25 mmol) in thf (5 mL) was added, causing the formation of a white, microcrystalline precipitate. After 1 h, the product was collected by filtration, washed with diethyl ether and dried in vacuo. Yield: 0.092 g (59%). Anal. calc. for C16H32F6GeN4O6S2 (627.2): C, 30.65; H, 5.14; N, 8.93. Found: C, 30.81; H, 5.17; N, 8.86%. 1H NMR (CD3CN, 298 K): 1.96 (s, [4H], NCH2CH2), 2.56 (br s, [12H], NCH3), 2.94–2.99 (v br, [16H], overlapping NCH2CH2CH2 and NCH2CH2N). 19F{1H} NMR (CD3CN, 298 K): −79.4 (O3SCF3). 1H NMR (DMF-d7, 298 K): 2.09 (quintet, [4H], 3JHH = 6.3 Hz, NCH2CH2), 2.68 (br s, [12H], NCH3), 3.08 (v br, [8H], NCH2CH2CH2) 3.21 (br s, [8H], NCH2CH2N). 19F{1H} NMR (DMF-d7, 298 K): −79.38 (O3SCF3). IR (Nujol/cm−1): 517m, 574m, 592w, 639s, 743w, 757w, 802w, 1011m, 1034s, 1160s, 1226m, 1256s, 1278s, 1354m.
[Ge(Me4cyclen)][GeCl3]2
[GeCl2(dioxane)] (0.104 g, 0.45 mmol) was suspended in CH2Cl2 (20 mL) and a solution of Me4cyclen (0.035 g, 0.15 mmol) in CH2Cl2 (10 mL) was added with stirring, giving a dense white suspension. After stirring at room temperature for 2 h, the product was collected by filtration, washed with Et2O and dried in vacuo. Yield: 0.048 g (48%). Anal. calc. for: C12H28Cl6Ge3N4 (658.9): C, 21.87; H, 4.28; N, 8.50. Found: C, 22.02; H, 4.19; N, 8.41%. 1H NMR (CD3CN, 298 K): 2.78 (s, [12H], NCH3), 3.20–3.38 (m, [16H], NCH2). IR (Nujol/cm−1): 277s, vbr [GeCl3]−, 317s, 413w, 472m, 547m, 737s, 747s, 791m, 917s, 945m, 958s, 1014s, 1024s, 1051s, 1064s, 1151m, 1262s, 1275s, 1298s.
[Ge(Me3tacn)][O3SCF3]2
[GeCl2(dioxane)] (0.059 g, 0.26 mmol) was suspended in CH2Cl2 (10 mL) and a solution of Me3SiO3SCF3 (0.112 g, 0.50 mmol) in CH2Cl2 (10 mL) was added with stirring, giving a colourless solution. After 10 min Me3tacn (0.044 g, 0.26 mmol) was added, causing the formation of a white precipitate. After stirring for approximately 1 h, the product was collected by filtration and dried in vacuo. Yield: 0.085 g (62%). Anal. calc. for C11H21F6GeN3O6S2 (542.0): C, 24.38; H, 3.91; N, 7.75. Found: C, 24.51; H, 3.74; N, 7.84%. 1H NMR (CD3CN, 298 K): 3.02 (s, [9H], NCH3), 3.34–3.54 (m, [12H], NCH2). 19F{1H} NMR (CD3CN, 298 K): −79.4 (O3SCF3). IR (Nujol/cm−1): 420m, 451w, 516m, 573m, 639s, 739m, 785m, 898m, 982w, 994m, 1030s, 1049m, 1138m, 1167s, 1226s, 1259s.
Crystals of [Ge(Me3tacn)][O3SCF3]2·CH3CN suitable for X-ray diffraction were obtained by layering an acetonitrile solution with diethyl ether.
[Ge(Me3tacn)]Cl[O3SCF3]
In a similar reaction using a 1
:
1 molar ratio of [GeCl2(dioxane)] and Me3tacn, conducted in MeCN solution, the mixture was stirred at room temperature for ca. 3 h following addition of Me3SiO3SCF3, then concentrated in vacuo. This did not cause any precipitation, and the solution was layered with Et2O and stored in the freezer. Small rod-shaped crystals formed, which were found to be [Ge(Me3tacn)]Cl[O3SCF3] as identified by an X-ray crystal structure determination. Anal. calc. for C10H21ClF3GeN3O3S (428.4): C, 28.04; H, 4.94; N, 9.81. Found: C, 28.76; H, 4.85; N, 9.77%. 1H NMR (298 K, CD2Cl2): 2.94 (s, [9H], NCH3), 3.21–3.47 (m, [12H], CH2). (A second minor species is also evident in the NMR spectrum). 19F{1H} NMR (298 K, CD2Cl2): −79.4 (O3SCF3).
[Ge(Me3tacn)]Cl2
In a further reaction conducted in MeCN solution, the mixture was stirred at room temperature for ca. 15 min following addition of Me3SiO3SCF3, then concentrated in vacuo. This caused the rapid precipitation of a white solid, which redissolved on warming. Storage of this solution in the freezer furnished colourless rod-shaped crystals which were found by X-ray crystallographic analysis to be [Ge(Me3tacn)]Cl2·MeCN.
[SiCl3(Me3tacn)][O3SCF3]
SiCl4 (0.170 g, 1.0 mmol) and Me3SiO3SCF3 (0.222 g, 1.0 mmol) were dissolved in CH2Cl2 (10 mL) and stirred for 5 min. A solution of Me3tacn (0.171 g, 1.0 mmol) in CH2Cl2 (5 mL) was added and the reaction was stirred for 16 h. After this time, a white solid had formed. This was collected by filtration and dried in vacuo. Yield: 0.204 g (45%). Anal. calc. for C10H21Cl3F3N3O3SSi (454.8): C, 26.40; H, 4.66; N, 9.24. Found: C, 26.61; H, 4.73; N, 9.25%. 1H NMR (295 K, CD3CN): 3.54–3.66 (m, [6H], NCH2), 3.31–3.41 (m, [6H], NCH2), 3.17 (s, [9H], NCH3). 13C{1H} NMR (295 K, CD3CN): 122.20 (q, 1JC–F = 320 Hz, CF3), 54.86 (CH2), 53.49 (CH3). 19F{1H} NMR (295 K, CD3CN): −78.7 (O3SCF3). IR (Nujol, cm−1): 231s, 428s (SiCl), 460s (SiCl), 497m, 517m, 574m, 601m, 637s, 754m, 899m, 967m, 998m, 1029s, 1053m, 1155s, 1225m.
Crystals were obtained by layering a concentrated CH2Cl2 solution with hexane.
[SiHCl2(Me3tacn)][BArF]
SiHCl3 (0.068 g, 0.50 mmol) and NaBArF (0.443 g, 0.50 mmol) were dissolved in toluene (10 mL) and stirred for 5 min. A solution of Me3tacn (0.085 g, 0.50 mmol) in toluene (5 mL) was added then the reaction was stirred for 4 h. After this time, volatiles were removed in vacuo and the solid extracted into CH2Cl2 (5 mL), filtered and hexane (30 mL) added to precipitate a white solid. Yield: 0.421 g (74%). Anal. calc. for C41H34BCl2F24N3Si (1134.12): C, 43.38; H, 3.02; N, 3.70. Found: C, 43.45; H, 3.11; N, 3.80%. 1H NMR (295 K, CD2Cl2): 7.74 (s, [8H], BArF H2/6), 7.59 (s, [4H], BArF H4), 4.78 (s, [1H], Si–H), 3.54–3.70 (m, [4H], NCH2), 3.26 (s, [3H], NCH3), 3.21 (s, [4H], NCH2), 3.12–3.17 (m, [4H], NCH2), 2.99 (s, [6H], NCH3). 13C{1H} NMR (295 K, CD2Cl2): 162.33 (q, 1JC–B = 49.8 Hz, BArF C1), 135.42 (CH, BArF C2/6), 129.48 (C, q, 1JC–F = 3.3 Hz, BArF C3/5), 125.22 (C, q, 1JC–F = 272 Hz, CF3), 118.11 (CH, BArF C4), 54.72, 53.77, 51.41, 50.45 (NCH2 and NCH3). IR (Nujol, cm−1): 449 m (SiCl), 480 m (SiCl), 683s, 744m, 838m, 888m, 899m, 1005m, 1056m, 1086m, 1114s, 1163s, 1280s, 1289s, 1356s, 1612w, 2137w (SiH).
[SiCl3(Me3tacn)][BArF]
Made similarly using SiCl4 (0.085 g, 0.50 mmol) in place of SiHCl3. Yield: 0.466 g (82%). Anal. calc. for C41H33BCl3F24N3Si (1168.9): C, 42.10; H, 2.85; N, 3.59. Found: C, 41.85; H, 3.08; N, 3.74%.
A concentrated CH2Cl2 solution of this complex layered with hexane deposited a few colourless crystals which were identified from an X-ray crystallographic study as [SiCl3(Me3tacn)]Cl. Attempts to prepare the latter directly from SiCl4 and Me3tacn in CH2Cl2 gave a pale yellow solid which was very poorly soluble in chlorocarbons and which was not analytically pure.
[SiCl3(pmdta)][BArF]
SiCl4 (0.085 g, 0.50 mmol) and Na[BArF] (0.443 g, 0.50 mmol) were dissolved in toluene (10 mL) and stirred for 5 min. A solution of pmdta (0.087 g, 0.50 mmol) in toluene (5 mL) was added, then the reaction was stirred for 4 h. After this time, volatiles were removed in vacuo and the solid extracted into CH2Cl2 (5 mL), filtered and hexane (30 mL) added to precipitate a white solid. Yield: 0.447 g (76%). Anal. calc. for C41H35BCl3F24N3Si (1170.58): C, 42.03; H, 3.01; N, 3.59. Found: C, 41.88; H, 3.12; N, 3.71%. 1H NMR (295 K, CD2Cl2): 7.72 (s, [8H], BArF H2/6), 7.57 (s, [4H], BArF H4), 2.76–2.98 (br s, [4H], NCH2), 2.65 (v br s, [16H], N(CH3)2 and NCH2), 2.35 (s, [3H], NCH3) ppm. 13C{1H} NMR (295 K, CD2Cl2): 162.37 (q, 1JC–B = 49.7 Hz, BArF C1), 135.41 (CH, BArF C2/6), 129.45 (C, q, 1JC–F = 3.3 Hz, BArF C3/5), 125.22 (C, q, 1JC–F = 272 Hz, CF3), 118.10 (CH, BArF C4), 57.91, 57.16 (CH2), 45.08 (N(CH3)2), 44.51 (NCH3). IR (Nujol cm−1): 448w, 506w (SiCl), 522w (SiCl), 682m, 713m, 889w, 1112s, 1143s, 1358s, 1367s.
Crystals were obtained by layering a concentrated CH2Cl2 solution with hexane.
[SiBr3(pmdta)][BArF]
SiBr4 (0.174 g, 0.50 mmol) and Na[BArF] (0.443 g, 0.50 mmol) were dissolved in toluene (10 mL) and stirred for 5 min. A solution of pmdta (0.087 g, 0.50 mmol) in toluene (5 mL) was added then the reaction was stirred for 4 h. After this time, volatiles were removed in vacuo and the solid extracted into CH2Cl2 (5 mL), filtered and hexane (30 mL) added to precipitate a white solid. Yield: 0.291 g (45%). Anal. calc. for C41H35BBr3F24N3Si (1303.93): C, 37.73; H, 2.71; N, 3.22. Found: C, 37.57; H, 2.80; N, 3.26%. 1H NMR (CD2Cl2): 7.72 (s, [8H], BArF H2/6), 7.57 (s, [4H], BArF H4), 2.76–2.98 (br s, [4H], NCH2), 2.65 (br s, [16H], N(CH3)2 and NCH2), 2.35 (s, [3H], NCH3). IR (Nujol, cm−1): 363 m (SiBr), 471w, 521w, 584w, 682s, 712s, 838m, 887m, 898m, 925w, 955w, 1112s, 1144s, 1279s, 1358s.
X-ray crystallography
Crystals were obtained as described above. Details of the crystallographic data collection and refinement are in Table 1. Diffractometer: Rigaku AFC12 goniometer equipped with an enhanced sensitivity (HG) Saturn724+ detector mounted at the window of an FR-E+ SuperBright molybdenum rotating anode generator (λ1 = 0.71073 Å) with VHF Varimax optics (70 or 100 μm focus). Cell determination, data collection, data reduction, cell refinement and absorption correction: CrystalClear-SM Expert 2.0 r7.4.15a Structure solution and refinement were carried out using WinGX or Olex2 and software packages within.15b–d No positional disorder was observed in complexes of [BArF]−, despite this being a common issue with weakly-coordinating anions containing CF3 groups, especially [BArF]−.16 [Ge(Me3tacn)]Cl2·MeCN crystallised as an inversion twin with a BASF of 0.21. Unusually large Z values were observed for [Ge(Me4cyclen)][O3SCF3]2·0.8MeCN and [SiCl3(Me3tacn)]Cl (10 and 24, respectively) which is explained by the presence of multiple cation units with very similar, but not identical, metrical parameters in the asymmetric unit. H atoms attached to C atoms were placed in geometrically assigned positions, with C–H distances of 0.95 Å (CH), 0.98 Å (CH3) or 0.99 Å (CH2) and refined using a riding model, with Uiso(H) = 1.2Ueq(C) (CH, CH2) or 1.5Ueq(C) (CH3). Si–H and N–H protons were located in the Fourier difference map and allowed to refine freely. enCIFer was used to prepare CIFs for publication.15e
Table 1 Selected X-ray crystallographic dataa
| Compound |
[Ge(Me3tacn)]-[O3SCF3]2·MeCN |
[Ge(Me4cyclen)]-[O3SCF3]2·0.8MeCN |
[Ge(Me3tacn)]-Cl[O3SCF3] |
[Ge(Me3tacn)]-Cl2·MeCN |
| Formula |
C13H24F6GeN4O6S2 |
C15.6H30.4F6GeN4.8O6S2 |
C10H21ClF3GeN3O3S |
C11H24Cl2GeN4 |
|
M/g mol–1 |
583.07 |
631.96 |
438.40 |
355.83 |
| Crystal system |
Monoclinic |
Tetragonal |
Monoclinic |
Orthorhombic |
| Space group (No.) |
P21/n (14) |
P4cc (103) |
P21/c (14) |
Pna21 (33) |
|
a/Å |
13.541(5) |
17.1253(3) |
8.1521(9) |
14.399(5) |
|
b/Å |
8.543(5) |
17.1253(3) |
13.9764(15) |
10.139(5) |
|
c/Å |
19.620(5) |
22.1160(10) |
14.2804(16) |
21.491(5) |
|
α/° |
90 |
90 |
90 |
90 |
|
β/° |
97.495(5) |
90 |
101.705(7) |
90 |
|
γ/° |
90 |
90 |
90 |
90 |
|
U/Å3 |
2250.3(17) |
6486.1(4) |
1593.2(3) |
3138(2) |
|
Z
|
4 |
10 (Z′ = 1.25) |
3 |
8 |
|
μ(Mo-Kα)/mm–1 |
1.634 |
1.425 |
2.267 |
2.284 |
|
F(000) |
1184 |
3236 |
872 |
1472 |
| Total reflections |
10 515 |
34 358 |
8862 |
11 548 |
| Unique reflections |
5123 |
7099 |
3647 |
5491 |
|
R
int
|
0.041 |
0.042 |
0.074 |
0.0823 |
| Goodness-of-fit on F2 |
1.036 |
1.030 |
0.987 |
1.025 |
R
1 b [Io > 2σ(Io)] |
0.037 |
0.054 |
0.047 |
0.061 |
|
R
1 (all data) |
0.050 |
0.071 |
0.060 |
0.108 |
wR2 b [Io> 2σ(Io)] |
0.082 |
0.131 |
0.108 |
0.103 |
| wR2 (all data) |
0.088 |
0.142 |
0.116 |
0.119 |
| Compound |
[SiCl3(Me3tacn)][O3SCF3] |
[SiCl3(Me3tacn)]Cl |
[SiCl3(pmdta)][BArF] |
|
Common items: T = 100 K; wavelength (Mo-Kα) = 0.71073 Å; θ(max) = 27.5°.
R
1 = ∑||Fσ| − |Fc||/∑|Fo|; wR2 = [∑w(Fo2 − Fc2)2/∑wFo2]1/2.
|
| Formula |
C10H21Cl3F3N3O3SSi |
C9H21Cl4N3Si·2/3(CH2Cl2) |
C41H35BCl3F24N3Si |
|
M/g mol–1 |
454.80 |
397.80 |
1170.97 |
| Crystal system |
Triclinic |
Monoclinic |
Orthorhombic |
| Space group (no.) |
P (2) |
C2/c (15) |
Pbca (61) |
|
a/Å |
6.997(2) |
34.475(8) |
17.728(5) |
|
b/Å |
10.820(4) |
26.707(6) |
19.613(6) |
|
c/Å |
11.974(4) |
11.820(3) |
26.662(8) |
|
α/° |
99.110(7) |
90 |
90 |
|
β/° |
93.245(5) |
106.684(5) |
90 |
|
γ/° |
92.108(8) |
90 |
90 |
|
U/Å3 |
892.7(5) |
10 425(4) |
9270(5) |
|
Z
|
2 |
24 (Z′ = 3) |
8 |
|
μ(Mo-Kα)/mm–1 |
0.743 |
0.946 |
0.357 |
|
F(000) |
468 |
4944 |
4704 |
| Total reflections |
7788 |
46 773 |
17 463 |
| Unique reflections |
4019 |
10 659 |
8124 |
|
R
int
|
0.019 |
0.114 |
0.070 |
| Goodness-of-fit on F2 |
1.042 |
1.107 |
1.176 |
R
1 b [Io > 2σ(Io)] |
0.032 |
0.094 |
0.097 |
|
R
1 (all data) |
0.039 |
0.121 |
0.147 |
wR2 b [Io> 2σ(Io)] |
0.069 |
0.227 |
0.137 |
| wR2 (all data) |
0.072 |
0.247 |
0.155 |
Results and discussion
Germanium(II) complexes
We have previously reported12 that reaction of GeBr2 with Me3tacn in anhydrous MeCN solution gives colourless [Ge(Me3tacn)]Br[GeBr3], containing unusual discrete three-coordinate [Ge(Me3tacn)]2+ dications (Ge–N = 2.124(3)–2.156(3) Å), with Br− and [GeBr3]− anions providing charge balance. We find that reaction of [GeCl2(dioxane)] with Me3tacn in anhydrous CH2Cl2 followed by addition of Me3SiO3SCF3 gave a colourless powder, [Ge(Me3tacn)][O3SCF3]2, subsequently obtained as colourless crystals of [Ge(Me3tacn)][O3SCF3]2·MeCN by recrystallisation from MeCN/Et2O. The structure (Fig. 1) also reveals a pyramidal GeN3 unit, however, in this species there are also weak directional Ge⋯O interactions from one oxygen in each triflate anion at 2.850(2) and 3.179(2) Å, well within the sum of vdW radii for O and Ge (3.79 Å).17
 |
| | Fig. 1 The X-ray structure of [Ge(Me3tacn)][O3SCF3]2·MeCN. Thermal ellipsoids are drawn at 50% probability, and hydrogen atoms omitted for clarity. Selected bond lengths (Å) and angles (°): N1–Ge1 = 2.084(2), N2–Ge1 = 2.106(2), N3–Ge1 = 2.089(2), O5⋯Ge1 = 2.850(2), O3⋯Ge1 = 3.179(2), N1–Ge1–N3 = 82.73(8), N1–Ge1–N2 = 82.84(8), N3–Ge1–N2 = 83.23(9). | |
While there is no evidence for 2
:
1 Me3tacn
:
Ge species (presumably due to steric clashing of the Me groups on the relatively small Ge(II) centre), the anions present in the products proved to be very sensitive to the reaction conditions; if the reaction of [GeCl2(dioxane)], Me3tacn and Me3SiO3SCF3 was conducted in MeCN solution as described in the Experimental section, concentrated in vacuo, and the solution layered with Et2O, the product was isolated as rod-like crystals of [Ge(Me3tacn)]Cl[O3SCF3]. The X-ray structure of this species (Fig. 2) shows the complex forms a weakly associated dimer in the solid state via the chloride bridges (Ge⋯Cl = 3.0254(9), 3.214(1) Å) and with a similar pyramidal ‘GeII(Me3tacn)’ core. These Ge⋯Cl interactions are substantially within the sum of vdW radii for Ge and Cl (4.11 Å). One κ1-coordinated triflate completes a distorted six-coordinate environment at each germanium centre.
 |
| | Fig. 2 The X-ray structure of [Ge(Me3tacn)]Cl[O3SCF3] showing the dimeric unit. Thermal ellipsoids are drawn at 50% probability, and hydrogen atoms omitted for clarity. Selected bond lengths (Å) and angles (°): N1–Ge1 = 2.119(3), N2–Ge1 = 2.139(3), N3–Ge1 = 2.130(2), Cl1⋯Ge1 = 3.0254(9), O1⋯Ge1 = 3.381(2), Cl1i⋯Ge1 3.214(1), N1–Ge1–N3 = 82.48(10), N1–Ge1–N2 = 81.63(10), N3–Ge1–N2 = 80.98(10). | |
The same reaction conducted in MeCN solution, but worked up after 15 min and placed in a freezer, deposited a few rod-like crystals that were identified as [Ge(Me3tacn)]Cl2·MeCN by X-ray crystallography (Fig. 3). In this case the ‘GeII(Me3tacn)’ core has two long contacts to the chlorides at 3.028(4) and 3.028(3) Å. The closest intermolecular contact is to a chloride of an adjacent molecule, but the Ge⋯Cl distance is the same as the sum of vdW radii for Ge and Cl (within experimental error), most likely a consequence of crystal packing.
 |
| | Fig. 3 The X-ray structure of [Ge(Me3tacn)]Cl2·MeCN showing the Ge1-centred molecule. The crystallographically independent Ge2-centred molecule is very similar. Thermal ellipsoids are drawn at 50% probability, and hydrogen atoms omitted for clarity Selected bond lengths (Å) and angles (°): N1–Ge1 = 2.124(10), N2–Ge1 = 2.147(10), N3–Ge1 = 2.154(9), Cl1⋯Ge1 = 3.028(4), Cl2⋯Ge1 = 3.028(3), N1–Ge1–N3 = 80.9(3), N1–Ge1–N2 = 81.2(4), N3–Ge1–N2 = 80.8(4). | |
Comparison of the Ge–N distances in this series of complexes shows only small differences as a function of the anion(s) present, suggesting that the structures are dominated by the ‘GeII(Me3tacn)’ core. All of the Ge–N distances are considerably longer than the sum of the covalent radii (1.85 Å),18 but well within the sum of the van der Waals radii (3.66 Å).17
The spectroscopic data provide very limited information; the IR spectra show the Me3tacn and the [O3SCF3]− (when present), whilst the 1H NMR spectra show small high frequency shifts corresponding to coordinated Me3tacn. The complexes are extremely sensitive to hydrolysis by trace water, readily forming protonated Me3tacn.
The reaction of [GeCl2(dioxane)] and Me3SiO3SCF3 in thf followed by addition of Me4cyclam gave [Ge(Me4cyclam)][O3SCF3]2. Attempts to obtain crystals of this complex were unsuccessful with recrystallisation from MeCN/Et2O or CH2Cl2/Et2O giving [Me4cyclamH2][O3SCF3]2 (identified crystallographically). We reported the structure of [Ge(Me4cyclam)][GeCl3]2 in our preliminary communication,12 which revealed an essentially coplanar N4 with the Ge out of the plane by 0.83 Å, and with no significant interaction with the anions. The data also revealed a spread of Ge–N distances (2.151(2)–2.349(2) Å), suggesting germanium(II) is not a good fit to the relatively large 14-membered macrocycle cavity; this may correlate with the very ready hydrolysis in solution.
Replacing the 14-membered Me4cyclam ring by the 12-membered Me4cyclen (1,4,7,10-tetramethyl-1,4,7,10-tetraazacyclotetradecane) gave colourless [Ge(Me4cyclen)][O3SCF3]2. Crystals of [Ge(Me4cyclen)][O3SCF3]2·0.8CH3CN suitable for X-ray diffraction were obtained by layering an acetonitrile solution of the complex with diethyl ether. The structure (Fig. 4) also shows the Ge(II) centre coordinated to a tetradentate Me4cyclen macrocycle with the Ge–N bonds alternating short-long-short-long around the ring, Ge–N = 2.165(6)–2.244(5) Å, with the Ge lying 1.009(3) Å above the mean N4 plane. In both complexes the methyl substituents on nitrogen are directed to the same side of the plane as the germanium centre. There are no significant interactions to the triflate anions, therefore, the germanium is in a highly distorted square planar, or tetragonal pyramidal, environment.
 |
| | Fig. 4 The X-ray structure of the dication present in [Ge(Me4cyclen)][O3SCF3]2·0.8CH3CN showing the Ge1-containing molecule. Thermal ellipsoids are drawn at 50% probability, and hydrogen atoms omitted for clarity. Selected bond lengths (Å) and angles (°): Ge1–N1 = 2.244(5), Ge1–N2 = 2.168(9), Ge1–N3 = 2.206(6), Ge1–N4 = 2.165(6), N1–Ge1–N3 = 131.8(2), N2–Ge1–N4 = 118.5(3), N2–Ge1–N1 = 78.2(2), N2–Ge1–N3 = 77.6(3), N4–Ge1–N1 = 77.8(2), N4–Ge1–N3 = 78.2(2). Symmetry codes: (i) x, y, 0.5 + z; (ii) −x, 1 − y, 0.5 + z. | |
The reaction of [GeCl2(dioxane)] in CH2Cl2 with Me4cyclen in a 3
:
1 molar ratio gave the corresponding [Ge(Me4cyclen)][GeCl3]2 which was less stable in solution.
Silicon(IV) complexes
The reaction of SiCl4, Me3tacn and Me3SiO3SCF3 in anhydrous CH2Cl2 solution produced [SiCl3(Me3tacn)][O3SCF3], which is much more hydrolytically sensitive than the [SiF3(Me3tacn)][SiF5] salt.11 Crystals of this chloro-complex were obtained by layering a concentrated CH2Cl2 solution with hexane. The structure of the cation shows the expected fac-octahedral coordination (Fig. 5). Comparison with the [SiF3(Me3tacn)]+ cation shows negligible differences between the Si–N distances.
 |
| | Fig. 5 View of the cation present in [SiCl3(Me3tacn)][O3SCF3]. Thermal ellipsoids are drawn at 50% probability, hydrogen atoms omitted for clarity. Selected bond lengths (Å) and angles (°): Si1–Cl1 = 2.1867(9), Si1–Cl2 = 2.1688(8), Si1–Cl3 = 2.1416(9), Si1–N1 = 2.010(2), Si1–N2 = 2.013(2), Si1–N3 = 2.026(2); N1–Si1–N2 = 85.61(7), N2–Si1–N3 = 84.70(6), N1–Si1–N3 = 85.37(6), Cl1–Si1–Cl2 = 91.79(4), Cl1–Si1–Cl3 = 92.18(3), Cl2–Si1–Cl3 = 92.76(3). | |
The corresponding [SiCl3(Me3tacn)][BArF] was obtained by reacting SiCl4 and Na[BArF] in toluene, followed by addition of a solution of Me3tacn. As we have described elsewhere,19 if the reagents are added simultaneously, the product is the sodium complex of the ligand, rather than the silicon cation. Crystals of [SiCl3(Me3tacn)][BArF] were not obtained, however, a concentrated CH2Cl2 solution of the [BArF]− salt, layered with hexane, produced a few colourless crystals identified by an X-ray structure determination as [SiCl3(Me3tacn)]Cl (see Fig. S1 in ESI†) which separate adventitiously due to the lower solubility of this salt. Direct reaction of SiCl4 and Me3tacn in CH2Cl2 resulted in precipitation of a pale yellow solid containing the same [SiCl3(Me3tacn)]Cl, however we have been unable to obtain it in analytically pure form by this route.
The 1H NMR spectrum of [SiCl3(Me3tacn)]+ in CD3CN at 298 K shows sharp second order multiplets characteristic of symmetrical fac-coordinated Me3tacn in solution.20
Similar reaction of SiHCl3 with Na[BArF] in toluene, followed by addition of Me3tacn, produced the corresponding dichlorosilane complex, [SiHCl2(Me3tacn)][BArF]. The presence of the Si–H group is shown by a singlet in the 1H NMR spectrum at δ = 4.78 and by ν(SiH) in the IR spectrum at 2137 cm−1. The presence of the fac-SiHCl2 removes the three-fold symmetry of the Me3tacn found in [SiCl3(Me3tacn)]+, and this is reflected in both the 1H and 13C{1H} NMR spectra, which show two δ(Me) resonances and corresponding splitting of the NCH2 resonances. Attempts to determine the structure of this complex have been unsuccessful. Poor quality crystals were obtained, but structure solution showed disordered [SiCl3(Me3tacn)]+ and [SiHCl2(Me3tacn)]+ were both present (note that [SiCl3(Me3tacn)]+ is not present in the NMR spectra of the bulk product). Disproportionation of silane complexes of amine ligands has been noted in other systems, and presumably occurs here slowly over the time taken to grow crystals from the [SiHCl2(Me3tacn)]+ solution.21
Finally, two complexes of the linear triamine, Me2NCH2CH2N(Me)CH2CH2NMe2 (pmdta), [SiX3(pmdta)][BArF] (X = Cl or Br) were isolated by reacting the appropriate SiX4 with Na[BArF] in toluene, followed by addition of pmdta. The X-ray crystal structure of the chloride reveals a mer-geometry (Fig. 6) which contrasts with the fac arrangement found in the Me3tacn complexes. The geometry of the [SiCl3(pmdta)]+ cation is close to octahedral, and the Si–N and Si–Cl distances are little different from those found in [SiCl3(Me3tacn)]+ despite the different donor arrangements. The geometry is also similar to that found in mer-[SiHCl2(pmdta)]+ (which has H trans to Cl).22
 |
| | Fig. 6 View of the cation in [SiCl3(pmdta)][BArF]. Thermal ellipsoids are drawn at 50% probability and hydrogen atoms are omitted for clarity. Selected bond lengths (Å) and angles (°): Si1–Cl1 = 2.147(2), Si1–Cl2 = 2.124(2), Si1–Cl3 = 2.184(2), Si1–N1 = 2.059(5), Si1–N2 = 2.028(5), Si1–N3 = 2.075(5); N1–Si1–N2 = 85.6(2), N2–Si1–N3 = 85.0(2) Cl1–Si1–Cl2 = 91.12(9), Cl2–Si1–Cl3 = 89.82(9). | |
The spectroscopic data are unexceptional, but consistent with the mer geometries, although it is notable that the terminal –NMe2 groups appear as a broad singlet rather than the two resonances expected due to the inequivalence produced by the central –NMe group lying out of the N3Cl plane. The ease of formation of the [SiX3(pmdta)]+ cations (X3 = Cl3, Br3, HCl2) is in contrast with the κ2-coordinated pmdta adduct formed with SiF4, reflecting the much higher Si–F bond strength.11
Conclusions
Two series of complexes with neutral aza-macrocyclic coordination to Ge(II) and Si(IV) are reported and structurally characterised. The hydrolytically sensitive Ge(II) triaza macrocyclic complexes show pyramidal GeN3 coordination with very weak, but variable, interactions from the chloride and triflate anions. This contrasts with the ‘naked’ dication identified in the previously reported [Ge(Me3tacn)]Br[GeBr3].12 The tetra-aza macrocyclic complexes of Ge(II) give GeN4 dications in highly distorted square planar geometries, with no significant anion interactions towards Ge(II).
The triaza ligand complexes of Si(IV), formed by halide abstraction using either Me3SiO3SCF3 or Na[BArF], adopt distorted octahedral coordination geometries, and the trichloro-, tribromo- and hydridodichloro-species reported here are significantly more readily hydrolysed than [SiF3(Me3tacn)]+.11
Acknowledgements
We thank EPSRC for support (EP/I010890/1 and EP/I033394/1). The SCFED Project (http://www.scfed.net) is a multidisciplinary collaboration of British universities investigating the fundamental and applied aspects of supercritical fluids.
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Footnote |
| † Electronic supplementary information (ESI) available: CCDC 1430051 ([Ge(Me3tacn)][O3SCF3]2·MeCN), 1430052 ([Ge(Me4cyclen)][O3SCF3]2·0.8MeCN), 1430053 ([Ge(Me3tacn)]Cl[O3SCF3]2), 1430054 ([Ge(Me3tacn)]Cl2·MeCN), 1430055 ([SiCl3(Me3tacn)][O3SCF3]), 1430056 ([SiCl3(Me3tacn)]Cl) and 1430057 ([SiCl3(pmdta)][BArF]). For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5dt03941j |
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