Synthesis and crystal structures of trimethylindium adducts with bidentate and macrocyclic tertiary amines

Kathleen M. Coward a, Anthony C. Jones *a, Alexander Steiner a, Jamie F. Bickley a, Lesley M. Smith b and Martyn E. Pemble c
aDepartment of Chemistry, University of Liverpool, Liverpool, UK L69 7ZD. Fax: 0151 493 2441;; E-mail: tony@tjconsultancy.demon.co.uk
bEpichem Limited, Power Road, Bromborough, Wirral, Merseyside, UK CH62 3QF
cDepartment of Chemistry, University of Salford, Salford, UK M5 4WT

Received (in Cambridge, UK) 23rd August 2000 , Accepted 27th October 2000

First published on 13th December 2000


Abstract

The structures of trimethylindium (Me3In) adducts with the bidentate tertiary amine N,N,N[hair space]′,N[hair space]′-tetramethyl-4,4′-methylenebis(aniline)[MBDA] and the macrocyclic amines 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane [N4-aza crown] and 1,4,7,10,13,16-hexamethyl-1,4,7,10,13,16-hexaazacyclooctadecane [N6-aza crown] have been determined by single crystal X-ray diffraction. The adducts have the following stoichiometries, Me3In·2MBDA 1, 2Me3In·MBDA 2, 4Me3In·N4-aza crown 3 and 6Me3In·N6-aza crown 4. Compound 1 contains five-coordinate Me3In in a trigonal bipyramidal configuration and displays the longest In–N bond lengths yet reported (2.720(4), 2.865 Å); 2–4 contain four-coordinate Me3In molecules in a tetrahedral configuration. Compounds 1–4 can be used as intermediate adducts in the adduct purification of Me3In for use in the MOVPE (metal organic vapour phase epitaxy) of InP and related III–V semiconductors.


1 Introduction

Tertiary amine adducts of trimethylindium (Me3In) have been known for many years,1 but relatively little structural information exists for these compounds. Recently there has been revived interest in trimethylindium–trialkylamine adducts as they are useful both as precursors in the metal organic vapour phase epitaxy (MOVPE) of InP and related III–V semiconductors,2,3 and in the purification of Me3In for subsequent use in MOVPE.4 For instance, the volatile adducts Me3In·NR3 (R = Me or Et) have been used as precursors for the MOVPE of InP,2,3 whilst the less volatile adduct 2Me3In· MBDA (MBDA = N,N,N[hair space]′,N[hair space]′-tetramethyl-4,4′-methylenebis(aniline)) has been used for purification of Me3In by mild thermal dissociation of the adduct.4,5

The amine ligand used in adduct purification must form a relatively weak donor–acceptor bond with the metal alkyl, allowing thermal dissociation of the adduct at relatively low temperatures (<150 °C) and must also be significantly less volatile than the liberated organometallic compound to allow easy separation.6 There are relatively few nitrogen donors which fulfil these criteria, for example the adducts Me3In·NMe3, Me3In·NEt3[hair space]2,3 and Me3In·N(CH2CH2)3N[hair space]7 all volatilise without appreciable dissociation. However, quantitative yields of high purity Me3In have been obtained by thermal dissociation of the 2Me3In·MBDA adduct.4,5

The rapid growth of MOVPE as a production technology for optoelectronic devices based on AlGaAs, AlGaInAs and AlGaInP is placing increasingly stringent requirements on the purity of the Group III metal organic precursor. Trace oxygen is a particular problem in Al-containing III–V devices, seriously degrading luminescence efficiency,8 and diethyl ether (a common solvent in organometallic synthesis) has been identified as a major source of oxygen contamination in III–V materials grown by MOCVD.9 It is therefore necessary completely to eliminate diethyl ether from the metal organic synthesis route. Recently we have shown that ultra high purity Me3In, essentially free from oxygen impurities, can be obtained by synthesis of the compound in a hydrocarbon solvent, followed by adduct purification using MBDA.10 Device data have been reported for a high quality low-oxygen content InAlGaAs GRINSCH laser structure grown by MOVPE using Me3In purified by thermal dissociation of Me3In·2MBDA. In this paper full structural details are given for the adducts Me3In·2MBDA 1 and 2Me3In·MBDA 2.

We have previously shown that the macrocyclic amines 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclooctadecane (N4-aza crown) and 1,4,7,10,13,16-hexamethyl-1,4,7,10,13,16-hexaazacyclooctadecane (N6-aza crown) (Fig. 1) form adducts which dissociate at low/moderate temperatures with triethylgallium,11 triisopropylgallium,11 and dimethylzinc.12 In this paper we report the synthesis and full structural characterisation of the analogous trimethylindium compounds, 4Me3In·N4-aza crown 3 and 6Me3In·N6-aza crown 4, and show that 1–4 also dissociate at relatively low temperature to liberate base-free Me3In. Although adducts between R3Ga and R3Al and macrocyclic amines have been reported,13–15 very few analogous Me3In adducts have been reported[hair space]16 and structural data are scarce.


Bidentate and macrocyclic tertiary amines used in this study: (a) MBDA, (b) N4-aza crown and (c) N6-aza crown.
Fig. 1 Bidentate and macrocyclic tertiary amines used in this study: (a) MBDA, (b) N4-aza crown and (c) N6-aza crown.

2 Experimental

General techniques

Trimethylindium was supplied by Epichem Limited. The nitrogen donor ligands used were MBDA, N4-aza crown and N6-aza crown. All were purchased from Aldrich Chemical Co., dried by distillation off sodium wire and deoxygenated before use.

1H NMR spectroscopy was carried out using a Bruker 300 spectrometer and infrared spectroscopy on a Perkin-Elmer 1000 infrared Fourier Transform spectrometer using Nujol mulls between NaCl plates. Elemental microanalyses were carried out by the Chemistry Department service at Liverpool University.

Adduct synthesis

The same general synthesis method was used for compounds 1–4. This involved addition of the amine [MBDA (0.5 mol equivalent, 2 mol equivalent), N4-aza crown (0.25 mol equivalent) or N6-aza crown (0.17 mol equivalent)] to a stirred suspension of Me3In (1 mol equivalent) in toluene. Removal of the toluene in vacuo gave 1–4 as crystalline solids which were characterised by 1H NMR, IR spectroscopy, elemental microanalysis and single crystal X-ray diffraction.
Me3In·2MBDA 1. Colourless crystalline solid. mp 71–72 °C. 1H NMR (C6D6, 300 MHz, 20 °C): δ −0.19[s, 9H, InCH3], 2.37[s, 24H, NCH3], 3.75[s, 4H, CCH2C] and 6.80[m, 16H, C6H4]. IR (cm−1): 1613s, 1514s, 1347m, 1272w, 1221w, 1164m, 1142s, 947w, 920m, 852m, 810m, 795m and 677s. Found: C, 66.7; H, 8.10, N, 8.6%. Calc. for C37H53InN4: C, 66.45; H, 8.00; N, 8.38%.
2Me3In·MBDA 2. Colourless crystalline solid. mp 79–80 °C. 1H NMR (C6D6, 300 MHz, 20 °C): δ −0.19[s, 18H, InCH3], 2.37[s, 12H, NCH3], 3.75[s, 2H, CCH2C] and 6.8[m, 8H, C6H4]. IR (cm−1): 1613s, 1514s, 1347m, 1272w, 1221w, 1164m, 1142s, 947w, 920m, 852m, 810m, 795m and 677s. Found: C, 47.77; H, 7.07; N, 4.79%. Calc. for C23H40In2N2: C, 48.09; H, 7.03; N, 4.88%.
4Me3In·N4-aza crown 3. Colourless crystalline solid. mp 181–182 °C. 1H NMR (C6D6, 300 MHz, 20 °C): δ 0.00[s, 36H, InCH3], 1.25[quintet, 4H, CH2CH2CH2], 1.95[s, 4H, NCH3] and 2.20[broad s, 16H, NCH2CH2CH2N, NCH2CH2N]. IR (cm−1): 2267w, 1608w, 1388m, 1329w, 1285w, 1215m, 1183m, 1148s, 1138m, 1089m, 1036s, 1027s, 1022m, 948w, 883w, 832w and 682s. Found: C, 34.73; H, 7.47; N, 5.80%. Calc. for C13H34In2N2: C, 34.84; H, 7.66; N, 6.25%.
6Me3In·N6-aza crown 4. Colourless crystalline solid. mp 103–104 °C. 1H NMR (C6D6, 300 MHz, 20 °C): δ −0.12[s, 36H, InCH3], 1.95[s, 18H, NCH3] and 2.51[broad s, 24H, NCH2CH2N]. IR (cm−1): 2274w, 1648w, 1302m, 1285w, 1210m, 1142m, 1121w, 1091m, 1067w, 1022m, 992m, 947w, 917m, 858w, 787w and 685s. Found: C, 33.30; H, 7.50; N, 6.7%. Calc. for C6H16InN: C, 33.19; H, 7.44; N, 6.45%.

Single crystal X-ray diffraction

Single crystals of compounds 1–4 suitable for X-ray diffraction were obtained by slow recrystallisation of each adduct from toluene. Crystallographic data were recorded on a STOE-IPDS diffractometer using graphite monochromated Mo-Kα radiation (λ = 0.71073 Å), T = 200 K. Structures were solved by Direct Methods and refined by full-matrix least squares against F[hair space]2 using all data.17 Crystal and data collection parameters are given in Table 1.
Table 1 Crystal and data collection parameters for Me3In·2MBDA 1, 2Me3In·MBDA 2, 4Me3In·N4-aza crown 3 and 6Me3In·N6-aza crown 4
  1 2 3 4
Empirical formula C37H53InN4 C23H40In2N2 C26H64In4N4 C36H96In6N6
Formula weight 668.76 574.29 892.22 1302.30
Crystal system Triclinic Monoclinic Monoclinic Monoclinic
Space group P[1 with combining macron] P21/c P21/n P21/c
a 10.641(5) 18.113(3) 7.8656(11) 10.6624(16)
b 10.763(4) 8.3668(7) 18.871(3) 22.856(3)
c 16.634(4) 18.058(3) 12.6821(18) 11.6461(17)
α 108.27(3)      
β 91.13(4) 106.182(18) 96.714(17) 108.184(17)
γ 105.45(4)      
V3 1732.5(11) 2628.3(6) 1869.5(5) 2696.5(7)
Z 2 4 4 2
μ/mm−1 0.637 1.621 2.266 2.355
Reflections collected 9330 16126 10131 16905
Reflections unique (Rint) 4310 (0.0813) 4152 (0.0506) 2531 (0.0581) 4251 (0.0443)
R1 [I > 2σ(I[hair space])] 0.0370 0.0317 0.0640 0.0256
wR2 (all data) 0.0809 0.0805 0.1780 0.0580


CCDC reference number 186/2258.

See http://www.rsc.org/suppdata/dt/b0/b008600m/ for crystallographic files in .cif format.

3 Results and discussion

Structures of Me3In·2MBDA 1 and 2Me3In·MBDA 2

The crystal structures of compounds 1 and 2 are shown in Figs. 2 and 3, whilst selected bond lengths and angles are given in Table 2.
Table 2 Selected bond lengths (Å) and angles (°) for Me3In·2MBDA 1 and 2Me3In·MBDA 2
1 2
In(1)–C(3) 2.157(5) In(1)–C(1) 2.167(4)
In(1)–C(1) 2.164(5) In(1)–C(2) 2.155(5)
In(1)–C(2) 2.189(5) In(1)–C(3) 2.172(4)
In(1)–N(1) 2.720(4) In(2)–C(4) 2.168(5)
In(1)–N(3) 2.865(4) In(2)–C(5) 2.165(5)
    In(2)–C(6) 2.171(6)
    In(1)–N(1) 2.446(3)
    In(2)–N(2) 2.462(4)
       
C(3)–In(1)–C(1) 121.1(2) C(2)–In(1)–C(3) 120.17(19)
C(3)–In(1)–C(2) 121.5(2) C(2)–In(1)–C(1) 116.2(2)
C(2)–In(1)–C(2) 117.3(2) C(3)–In(1)–C(1) 116.35(18)
C(3)–In(1)–N(1)  90.99(16) C(4)–In(2)–C(5) 117.4(3)
C(1)–In(1)–N(1)  90.82(16) C(4)–In(2)–C(6) 118.5(2)
C(2)–In(1)–N(1)  92.03(16) C(5)–In(2)–C(6) 117.2(3)
C(3)–In(1)–N(3)  89.51(16) N(1)–In(1)–C(1) 101.42(14)
C(1)–In(1)–N(3)  88.72(16) N(1)–In(1)–C(2)  98.69(15)
C(2)–In(1)–N(3)  87.91(16) N(1)–In(1)–C(3)  97.07(14)
N(1)–In(1)–N(3) 179.45(12) N(2)–In(2)–C(4) 100.13(18)
    N(2)–In(2)–C(5)  97.0(2)
    N(2)–In(2)–C(6)  99.26(18)



Crystal structure of Me3In·2MBDA 1.
Fig. 2 Crystal structure of Me3In·2MBDA 1.

Crystal structure of 2Me3In·MBDA 2.
Fig. 3 Crystal structure of 2Me3In·MBDA 2.

The structure of compound 1 is noteworthy in that the Me3In moiety is five-coordinate with the longest In–N bond lengths (2.720(4), 2.865(4) Å) reported to date. Only a few five-coordinate alkylindium adducts have been reported, and these generally involve chelating donor ligands (e.g. Me3In·Me2NCH2NMe2[hair space]18 and Me2InCl·2,2′-bipy[hair space]19) and structural data are scarce. The In–N bond lengths are significantly greater than those in the adducts Me3In·[upper bond 1 start]NHCMe2(CH2)3C[upper bond 1 end]Me2 and Me3In·NHMe(CH2)2NHMe·InMe3 which are 2.502(5) and 2.369(7) Å, respectively.7 In 1 the Me3In moiety is in a trigonal bipyramidal configuration with a linear N–In–N bond angle of 179.45(12)°, similar to the Me3In configuration in the polymeric complex [Me3In·N(CH2CH2)3N]x, which also displays very long In–N bond lengths (2.62 Å).7 The C–In–C bond angles in 1 of close to 120° are very close to those in pure unadducted Me3In, in which the Me3In exists in the trigonal planar configuration, providing further evidence of the very weak In–N interactions in 1.

The long In–N bond lengths in five-coordinate trigonal bipyramidal adducts such as 1 and [Me3In·(NCH2CH2)3N]x have been attributed[hair space]7 to the In being sp3d hybridised (i.e. donation of nitrogen lone pairs into a combination of 5pz and 5dz2 orbitals on In). These will be weaker interactions than donation into a single vacant sp3 hybrid orbital on In, as occurs in four-coordinate Me3In·L adducts.

In compound 2 the In–N lengths of 2.446(3) and 2.462(4) Å are significantly shorter than in 1, indicating a stronger In–N interaction. The Me3In is four-coordinate and exists in a distorted tetrahedral environment with N–In–C bond angles ranging from 97.0(2)° to 101.42(14)°, similar to those in Me3In·NHMe(CH2)2NHMe·InMe3 (98.8(4)–101.4(3)°) and Me3In·[upper bond 1 start]NHCMe2(CH2)3C[upper bond 1 end]Me2 (92.8(2)–109.3(2)°). The C–In–C bond angles in 2 (≈116°) are similar to those in Me3In· NHMe(CH2)2NHMe·InMe3 (≈116°) and Me3In·NHCMe2(CH2)3CMe2 (≈117.6°),7 which also display comparable In–N bond distances (2.37–2.50 Å).

The similarity in chemical shifts in the 1NMR data for 1 and 2 suggests that both compounds may be present in mixtures of Me3In and MBDA in solution. This may be similar to the case of mixtures of Et3Ga and N6-aza crown in which two separate species, 4Et3Ga·N6-aza crown and 6Et3Ga·N6-aza crown, were isolated from the same solution and characterised by X-ray diffraction.11

Structures of 4Me3In·N4-aza crown 3 and 6Me3In·N6-aza crown 4

The crystal structures of compounds 3 and 4 are shown in Figs. 4 and 5, respectively and selected bond distances and angles are given in Table 3. Each adduct displays the expected 4∶1 and 6∶1 Me3In∶ligand stoichiometries. In the case of 4 this contrasts with N6-aza crown complexes involving more bulky R3Ga moieties, such as 4PriGa·N6-aza crown where steric constraints limit the stoichiometry at 4∶1.11
Table 3 Selected bond lengths (Å) and angles (°) in 4Me3In·N4-aza crown 3 and 6Me3In·N6-aza crown 4
3 4
In(1)–C(1) 2.169(16) In(1)–C(1) 2.166(4)
In(1)–C(2) 2.158(17) In(1)–C(2) 2.169(4)
In(1)–C(3) 2.175(16) In(1)–C(3) 2.170(5)
In(2)–C(4) 2.170(17) In(2)–C(4) 2.168(5)
In(2)–C(5) 2.162(18) In(2)–C(5) 2.166(5)
In(2)–C(6) 2.180(17) In(2)–C(6) 2.169(6)
In(1)–N(1) 2.433(12) In(1)–N(1) 2.490(3)
In(2)–N(2) 2.427(11) In(2)–N(2) 2.462(3)
    In(3)–N(3) 2.449(3)
       
C(1)–In(1)–C(2) 118.1(7) C(1)–In(1)–C(2) 118.7(2)
C(1)–In(1)–C(3) 121.3(7) C(1)–In(1)–C(3) 113.97(19)
C(2)–In(1)–C(3) 113.8(8) C(2)–In(1)–C(3) 122.16(18)
C(6)–In(2)–C(5) 120.8(8) C(7)–In(3)–C(8) 120.4(2)
C(6)–In(2)–C(4) 120.9(7) C(7)–In(3)–C(9) 119.5(2)
C(4)–In(2)–C(5) 111.7(8) C(8)–In(3)–C(9) 113.1(2)
N(1)–In(1)–C(1)  95.9(6) N(1)–In(1)–C(1)  99.79(15)
N(1)–In(1)–C(2) 104.2(5) N(1)–In(1)–C(2)  97.86(14)
N(1)–In(1)–C(3)  96.4(6) N(1)–In(1)–C(3)  95.27(14)
N(2)–In(2)–C(4) 101.1(5) N(2)–In(2)–C(4) 101.85(17)
N(2)–In(2)–C(5)  99.3(6) N(2)–In(2)–C(5) 100.44(15)
N(2)–In(2)–C(6)  95.6(6) N(2)–In(2)–C(6)  97.87(16)



Crystal structure of 4Me3In·N4-aza crown 3.
Fig. 4 Crystal structure of 4Me3In·N4-aza crown 3.

Crystal structure of 6Me3In·N6-aza crown 4.
Fig. 5 Crystal structure of 6Me3In·N6-aza crown 4.

In compounds 3 and 4 the Me3In molecules exhibit distorted tetrahedral geometry, with C–In–N bond angles ranging from 95.6(6) to 104.2(5)° in 3 and 95.27(14)–101.85(17)° in 4, significantly less than the tetrahedral angle of 109°. These are entirely typical of C–In–N bond angles in tetrahedrally coordinated Me3In adducts, as shown by the comparative data for a range of Me3In–tertiary amine adducts given in Table 4. The In–N bond lengths in 3 and 4 are close to the In–N bond length in 2, and fairly typical for In–N bond lengths in an sp3 hybridised tetrahedral configuration (see Table 4). The In–N bond lengths in 2, 3 and 4 are significantly shorter than the In–N length in the sp3d hybridised complex 1. The In–N bond distance in 4 is very slightly longer than that in 3, presumably due to a slight increase in steric hindrance in the 6Me3In·N6-aza crown complex.

Table 4 Bond lengths (Å) and angles (°) for some Me3In–tertiary amine adducts
Compound In–N In–C C–In–C C–In–N Reference
Me3In·2MBDA 1 2.720(4), 2.865(4) 2.157(5)–2.189(5) 117.3(2)–121.5(2) 87.91(16)–92.03(16) This work
2Me3In·MBDA 2 2.446(3), 2.462(4) 2.165(5)–2.172(4) 116.2(2)–120.17(19) 97.0(2)–101.42(14) This work
4Me3In·N4-aza crown 3 2.427(11)–2.433(12) 2.158(17)–2.180(17) 111.7(8)–121.3(7) 95.6(6)–104.2(5) This work
6Me3In·N6-aza crown 4 2.449(3)–2.490(3) 2.166(4)–2.170(5) 113.1(2)–122.6(18) 95.27(14)–103.13(16) This work
Me3In·[upper bond 1 start]NHCMe2(CH2)3C[upper bond 1 end]Me2 2.502(5) 2.170(5)–2.174(6) 109.3(3)–118.9(3) 92.8(2)–109.3(2) 7
Me3In·NHMe(CH2)2NHMe·InMe3 2.369(7), 2.393(7) 2.147(10)–2.183(9) 113.0(4)–120.2(4) 96.3(3)–101.4(3) 7
[Me3In·N(CH2CH2)3N]x 2.62 2.172(7)–2.176(5) 119.4(2) 7


The Me3Al and Me3Ga analogues to 2 have been structurally characterised,13,14 and this allows us to make a direct comparison of M–N, M–C bond lengths, and various intramolecular angles in the R3M molecule (see Table 5). The most notable feature is that the M–N adduct bond length decreases in the order In > Ga > Al, in line with increasing Lewis acidity of the metal centre.20 The M–C bond lengths show a similar trend, decreasing in the order In > Ga ≈ Al, broadly consistent with increasing strength of the metal–carbon bond. The M–C bond lengths in the 4Me3Ga·N4-aza crown and 4Me3In·N4-aza crown adducts are close to those in the unadducted compounds, Me3Ga(g) (M–C: 1.967(2) Å)[hair space]21 and Me3In(s) (M–C: 2.16(4)–2.25(6) Å).22,23 However, the Al–C bond lengths of 1.960(5)–1.966(6) Å in 4Me3Al·N4-aza crown are slightly shorter than the terminal Al–C distances in the Me3Al dimer (1.99 Å).24 The C–M–N bond angle decreases in the order Al > Ga > In, with an increasing deviation from the tetrahedral angle of 109°.

Table 5 Bond lengths (Å) and angles (°) for Me3M·N4-aza crown adducts (M = Al, Ga or In)
Compound M–N M–C C–M–C C–M–N Reference
4Me3Al·N4-aza crown 2.093(3), 2.102(3) 1.960(5)–1.966(6) 102.8(2)–107.1(2) 13
4Me3Ga·N4-aza crown 2.182(4), 2.202(4) 1.970(6)–1.973(6) 113.0(3)–118.1(3) 101.0(2)–105.9(2) 14
4Me3In·N4-aza crown 2.433(12), 2.427(11) 2.158(17)–2.180(17) 111.7(8)–121.3(7)  95.6(6)–104.2(5) This work


Dissociation of Me3In–aza crown adducts

Complex 2 has previously been shown to liberate base free Me3In when heated at 80–130 °C in vacuo.4 Complexes 1, 3 and 4 were also found to liberate base-free Me3In (confirmed by 1H NMR spectroscopy) when heated at relatively low temperatures 80–115 °C under vacuum. A sample of crude Me3In containing high levels of MeI (18000 ppm, deriving from the Grignard-based synthesis route) was purified by thermal dissociation of the adducts 1–4 and it was shown that, in each case, the iodide impurity level was reduced to <10 ppm. Such a dramatic reduction can be attributed to formation of the involatile quaternary ammonium salt, R4N+I, resulting from reaction between the tertiary amine and MeI.25 It has previously been shown that MBDA is highly effective in removing trace metal impurities (e.g. Si, Zn, Mg) from Me3In,4 but removal of the organic impurity MeI is a useful additional advantage of tertiary amines in adduct purification processes.

4 Conclusion

The crystal structures of Me3In·2MBDA 1, 2Me3In·MBDA 2, 4Me3In·N4-aza crown 3 and 6Me3In·N6-aza crown 4 have been determined. Compound 1 is one of only two reported adducts containing five-coordinate Me3In, whereas 2–4 contain four-coordinate Me3In in a distorted tetrahedral configuration. The adducts 1–4 all liberate base-free Me3In at low/moderate temperatures and are suitable for adduct purification of Me3In for electronic applications.

Acknowledgements

We are very grateful to Epichem Limited for funding the work and for providing samples of Me3In. We also thank Mr S. A. Apter (University of Liverpool, UK) for provision of the microanalytical data.

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