Kristian L.
Mears
,
Malavika A.
Bhide
,
Caroline E.
Knapp
* and
Claire J.
Carmalt
*
Department of Chemistry, University College London, 20 Gordon Street, London, WC1H 0AJ, UK. E-mail: c.j.carmalt@ucl.ac.uk
First published on 1st December 2021
Amidoenoate (AME = {ethyl-3-(R-amido)but-2-enoate}) complexes of aluminium and gallium, of the type: [AlCl2(AMER)] R = iPr (1-Al); [AlCl(AMER)2] R = iPr (2-Al), Dip (3-Al); [GaCl2(AMER)] R = iPr (1-Ga) and [GaCl(AMER)2] R = iPr (2-Ga), Dip (3-Ga), have been synthesised (iPr = isopropyl, Dip = 2,6-diisopropylphenyl). The coordination chemistry of these complexes has been studied in relation to precursor suitability. Investigations into the reactivity of the aluminium and gallium amidoenoate complexes involved reactions with hydride sources including alkali metal hydride salts, alkylsilanes, and magnesium hydride species and magnesium(I) dimers. The isolation of alkyl metal amidoenoate precursors including an aluminium hydride amidoenoate, [AlH(AMEDip)2] (4-Al) and dimethyl gallium amidoenoates [GaMe2(AMEDip)] (4-Ga), [GaMe2(AMEiPr)] (5-Ga) concluded the synthetic studies. A selection of the isolated complexes were used as precursors for aerosol assisted chemical vapour deposition (AACVD) at 500 °C. Thin films of either amorphous Al2O3 or Ga2O3 were deposited and subsequently annealed at 1000 °C to improve the materials’ crystallinity. The films were characterised by X-ray diffraction (XRD), X-ray photoelectron spectroscopy (XPS), scanning electron microscopy (SEM), UV-visible (UV-vis) spectroscopy and energy dispersive X-ray analysis (EDXA).
Methods employed by synthetic chemists to control such parameters include varying the chemical nature of the complex by choosing specific ligands to perform certain functions. For example, incorporating per-fluorinated ligands at metal centres in order to achieve a precursor with high volatility,20 or choosing fluxional ligands, such as donor-functionalised alkoxides with hemi-labile properties to encourage gas-phase decomposition during CVD.21–23 Ligands which aid metal–oxide formation often include a source of oxygen such as diketonates and β-ketoiminates (BKIs), as shown in Fig. 1 (A and B respectively), have become well established ligands in the literature for metal complexes used to deposit oxide materials.24–29 One advantage the BKI ligand has over the nitrogen free β-diketonates is the option to incorporate various steric profiles at the N-position.
This ability to tune the steric profile within the metal's coordination centre is almost solely considered for stabilising complexes that require significant stabilisation due to an unusual oxidation state or kinetic instability,30,31 however these design principles are becoming more common in precursor synthesis. For example, the aminoenoate (HAME), (Fig. 1, C) includes a nitrogen donor that can be functionalised to incorporate varying steric bulk, as well as two oxygen atoms to afford a high inherent oxygen content, but amidoenoate (AME) ligands have yet to receive the same attention as other (O,N)-coordinating ligands, such as BKI motifs.
Previously, we have shown that AME ligands can act as oxygen saturated systems at zinc centres (Fig. 2, A–D) to form precursors which successfully converted to zinc oxide (ZnO) via AACVD.32,33 McElwee-White and co-workers have employed AMEs at tungsten centres (Fig. 2, E and F), generating a range of tungsten oxide precursors with interesting molecular geometries which afforded W:O ratio control in the resulting thin films depending on the deposition temperature used.34
Fig. 2 Previously reported zinc bis-amidoenoates (A and B), ethyl zinc amidoenoate dimers (C and D) and tungsten amidoenoate complexes (E and F).32–34 Differing steric profiles are highlighted in pink. |
As zinc and tungsten AME systems have been investigated previously and afforded viable oxide precursors, AME ligands at group 13 centres, such as aluminium and gallium may result in similarly successful precursors to these oxides, which have a range of applications including solar cells, abrasives and sensors.35,36 Here, we investigate AME ligands at aluminium and gallium centres as precursors towards aluminium oxide (α-Al2O3) or gallium oxide (β-Ga2O3) respectively.
As very few solution-based precursors towards aluminium oxide have been previously reported,37 we focused particularly on the synthesis of [Al(AME)] systems. For comparison with another important oxide material (β-Ga2O3), the analogous gallium complexes were also prepared, noting that precursors to gallium oxide often rely on alkoxides, diketonates and BKI systems.38,39
The aminoenoate pro-ligand bearing an iPr-group at the N-position (HAMEiPr) was synthesised according to previously reported literature,32 and the bulkier analogue bearing a Dip-substituent, Dip = 2,6-diisopropylphenyl (HAMEDip) was isolated following a similar procedure (ESI). Initially, the lithium salts of these compounds were generated from a 1:1 metathesis reaction with lithium silylamide etherate (Scheme 1, left). The resulting [Li(AMEiPr)] and [Li(AMEDip)] salts which were both isolated as white crystalline material in excellent yields (80% and 86% respectively) were initially reacted with aluminium trichloride. In order to probe the stability offered by the amidoenoate ligand with the least-bulky R-group (iPr), a 1:1 reaction of [Li(AMEiPr)] with AlCl3 was carried out (Scheme 1, route A) in diethyl ether and afforded [AlCl2(AMEiPr)] (1-Al) as a pale oil that was titurated in hexane to afford a white powder in good yield (69%). The molecular structures of complexes 1-Al–3-Al are shown in Fig. 3 and selected bond lengths and angles are shown in Table 1. The geometry of [AlCl2(AMEiPr)] at the aluminium centre was found to be tetrahedral (τ4 = 0.92).
1-Al | 2-Al | 3-Al | 1-Ga | 2-Ga | 3-Ga | |
---|---|---|---|---|---|---|
Bond lengths (Å) | ||||||
M–Cl(1) | 2.1287(5) | 2.2362(5) | 2.1969(5) | 2.1553(5) | 2.2443(5) | 2.2177(4) |
M–Cl(2) | 2.1178(5) | — | — | 2.1661(5) | — | — |
M–N(1) | 1.8721(11) | 1.9356(12) | 1.9746(12) | 1.9050(14) | 1.9506(16) | 1.9888(11) |
M–N(2) | — | 1.9338(12) | 1.9782(11) | — | 1.9510(16) | 1.9861(12) |
M–O(1) | 1.7689(9) | 1.8608(11) | 1.8477(10) | 1.8664(11) | 1.9960(14) | 1.9734(10) |
M–O(3) | — | 1.8545(11) | 1.8541(10) | — | 1.9807(14) | 1.9687(10) |
Bond angles (°) | ||||||
O(1)–M–N(1) | 100.43(5) | 91.15(5) | 90.20(5) | 100.92(5) | 91.03(6) | 91.41(4) |
N(1)–M–Cl(1) | 115.08(4) | 117.58 | 115.27(4) | 116.11(5) | 117.16(5) | 114.77(3) |
O(1)–M–O(3) | — | 174.14(5) | 176.34(5) | — | 172.85(6) | 178.95(5) |
N(1)–M–N(2) | — | 121.52(6) | 130.91(5) | — | 122.42(7) | 129.34(5) |
Cl(1)–M–Cl(2) | 109.48(2) | — | — | 108.96(2) | _ | — |
τ value | 0.92 | 0.87 | 0.76 | 0.96 | 0.84 | 0.83 |
Complex 1-Al represents the first example of a tetrahedral aluminium dichloride unit featuring a ligand that binds through both oxygen and nitrogen and was synthesised from the salt metathesis reaction of [Li(AMEiPr)] and AlCl3 (Scheme 1).
Two previous examples of aluminium dichlorides featuring (O,N)-binding ligands have been reported by Richards40 and Schulz,41 with the formulae [AlCl2{(OC(Me)CHC(Me)NC2H4NEt2)}] and [AlCl2{(OC(Me)C(H)C(Me)NC2H4NMe2)}] respectively, but are 5-coordinate complexes due to the extra donor functionality incorporated into the ligand.
All Al-heteroatom bonds in 1-Al were found to be significantly shorter than the 5-coordinate complexes reported by Richards and Schulz previously,40,41 which is likely a consequence of the comparatively electron deficient nature of the aluminum center in 1-Al. Complexes 2-Al and 3-Al both displayed a distorted trigonal bipyramidal geometry with a τ4 value of 0.87 for 2-Al and 0.76 for 3-Al, suggesting that the Dip-substituted amidoenoate ligands in 3-Al distort the geometry of the aluminium center significantly more than the iPr-substituents in 2-Al. The Al–Cl bond lengths (2.2362(5) Å and 2.1969(5) Å in 2-Al and 3-Al respectively) were similar to other 5-coordinate {Al–Cl} containing complexes bearing (O,N)-ligands.42–44 Following the successful isolation of (1–3)-Al, the heavier gallium analogues were targeted. Using similar routes (Scheme 1), the 1:1 and 1:2 reaction of GaCl3 and [Li(AMEiPr)] yielded complexes [GaCl2(AMEiPr)] (1-Ga) and [GaCl(AMEiPr)2] (2-Ga) as pale-yellow oils which could be titurated in hexane to give powders in good yields (62% and 63% respectively). [GaCl(AMEDip)2] (3-Ga), was isolated as a white powder in excellent yield (86%) from the salt metathesis of two equivalents of [Li(AMEDip)] and one equivalent of GaCl3. The geometries of complexes (1–3)-Ga were almost identical to those found for their aluminium analogues. Complex 1-Ga had a geometry similar to that of 1-Al, displaying a tetrahedral geometry with a τ4 value of 0.96 – only 4% distorted from a perfect tetrahedral geometry, whereas 1-Al had a distortion of 8%. Interestingly, the Ga–Cl(2) bond length (2.1661(5) Å) in 1-Ga was identical to that of a previously reported gallium bis-chlorido BKI complex with the formula [GaCl2(Me(O)C(H)C(NiPr)Me)].45
Complex 2-Ga featured a trigonal bipyramidal geometry, though slightly more distorted than the aluminium analogue with a τ5 value of 0.84 (3% more distorted than 2-Al). This complex also had the largest Ga–Cl(1) bond length of the set of {Ga–Cl} containing complexes presented in this study. The complex 3-Ga also displayed a trigonal bipyramidal geometry, though was less distorted than 3-Al. A further trend observed was that the complexes with the formula [MCl(AMEiPr)2], M = Al, Ga (2-Al and 2-Ga) featured the longest M–Cl(1) bond lengths, rather than the bulkier Dip-substituent containing system with the formula [MCl(AMEDip)2], M = Al, Ga (3-Al and 3-Ga). The result of this observation is proposed to be electronic, rather than steric in nature. The donating effect from the iPr group in 2-Al and 2-Ga likely affords a more basic amide and hence a stronger N-donor to the metal. The M–Cl bond lengthens as a result to stabilize the quantity of electron density at the metal center. For complexes 3-Al and 3-Ga, the bulkier Dip-substituents at the N-position are electron withdrawing, and so shorter M–Cl(1) bond lengths were observed, despite these complexes having to accommodate larger ligands in their coordination spheres.
In most cases, the M–O(1) bond lengths are shorter than the M–N(1) bond lengths in both the (1–3)-Al and (1–3)-Ga systems and is likely due to delocalisation in the ligand backbone (Table 1). Complex 2-Ga was the only case (for the complexes presented) where the M–O(1) bond length was longer than the M–N(1) bond length.45 This may be a consequence of gallium's slightly shorter covalent radius compared to aluminium, resulting in the lengthening of the M–O(1) bond to accommodate the two strongly donating NiPr groups, despite the oxophilic nature of the metal.
Scheme 2 Attempted formation of group 13 amidoenoate hydrides using alkali metal hydrides, silanes and magnesium hydride dimers. |
Complexes 3-Al and 3-Ga were chosen for the reactivity study as these complexes had the most distorted structures of the set of amidoenoate complexes synthesised (τ5 values of 0.76 and 0.83 for 3-Al and 3-Ga respectively) and hence, it was hypothesized that replacing the chloride for a smaller hydride in these systems may be an energetically favourable process and result in the desired {M–H} product.
Conventional hydride sources including metal hydride salts and silanes with varying acidity were attempted but did not result in the conversion to the group 13 hydride. Jones’ accessible magnesium hydride dimer46 was then employed in order to probe if the formation of an [MgCl(BDIDip)] complex would drive the metathesis, but this route also resulted in no conversion (either by NMR or product isolation). For the cases of routes 1 and 2 (Scheme 2), crystalline starting material of 3-Al or 3-Ga could be obtained. These results suggested that the (O,N)-coordinating bulky Dip-substituted amidoenoate ligands provided significant stability at the group 13 centers. Final attempts at abstracting the Cl-atom from the main group centres involved employing Jones’ low-valent Mg(I) complex,47 [Mg(BDIMes)]2 (Mes = mesityl), in order to either reduce the complexes to form [(AME)2M–M(AME)2] dimers or by installing [M–Mg] (M = Al, Ga) bonds. At elevated temperatures, these reactions resulted in some AME-complex decomposition (as evidenced by 1H NMR experiments – see ESI†). As functionalisation of the chloride to a hydride was not achieved, the reactivity study proceeded to investigate whether a group 13-hydride synthon could be used to synthesize a metal hydride bis-amidoenoate complex (Scheme 3).
One equivalent of HAMEDip dissolved in toluene and was added dropwise to half an equivalent of [GaH3(NMe3)] in hexane at −78 °C. However, the acid–base reaction between HAMEDip and [GaH3(NMe3)] resulted in no observable hydrogen evolution and eventually, decomposition of the gallium hydride to gallium metal occurred. Despite [GaH3(NMe3)] being a successful synthon for the isolation of other {Ga–H} containing precursors we have reported previously, such as [GaH(NMe3−x{CH2CH2O}x)2],48,49 the amine-stabilized gallane employed was not found to react with the aminoenoate pro-ligand. Despite the various temperature and solvent conditions attempted (which included keeping the reaction mixture at 0 °C for 12 hours, or using various solvents including toluene, hexane and diethyl ether), a gallium hydride bis-amidoenoate complex could not be isolated via this route.
In contrast, when one equivalent of HAMEDip was added to a cooled (−78 °C) solution of half an equivalent of [AlH3(NMe3)] in toluene, vigorous bubbling consistent with the formation of dihydrogen was observed instantly. This mixture was allowed to stir for 4 hours, and subsequent removal of all volatiles yielded a white powder. The powder was redissolved in warm hexane and after 24 hours, yielded the complex [AlH(AMEDip)2] (4-Al) as block-like colourless crystals (Fig. 4). 4-Al was found to adopt a trigonal bipyramidal geometry akin to that of its chloride analogue 3-Al, though as expected the τ5 value of the hydride had increased to 0.79, suggesting that the smaller H-group afforded a geometrically more stable complex. Selected bond lengths and angles for 4-Al are shown in Table 2.
Fig. 4 Molecular structure of [AlH(AMEDip)2] (4-Al). Thermal ellipsoids shown at 30%. Dip-substituents are in wireframe for clarity. |
Bond lengths (Å) | |
Al(1)–N(1) | 1.985(2) |
Al(1)–N(2) | 1.984(2) |
Al(1)–O(1) | 1.877(2) |
Al(1)–O(2) | 1.879(2) |
Bond angles (°) | |
O(1)–Al(1)–O(3) | 173.79(9) |
N(1)–Al(1)–N(2) | 126.48(9) |
O(1)–Al(1)–N(1) | 89.30(8) |
O(1)–Al(1)–N(2) | 87.55(8) |
O(3)–Al(1)–N(1) | 88.34(9) |
O(3)–Al(1)–N(2) | 89.24(8) |
Huang and co-workers have reported the only other {Al–H} containing complex stabilized by (O,N)-containing ligands, which featured β-ketoiminate (BKI) ligands and the same Dip-substituent at the N-position (formula [AlH(BKIDip)2]).44 Comparing the bond lengths in 4-Al and Huang's complex, both Al(1)–O(1) and Al(1)–O(3) bond lengths were significantly longer at 1.877(2) Å and 1.879(2) Å respectively, compared to 1.763(3) Å and 1.757(3) Å in [AlH(BKIDip)2]. However, the opposite was true for the Al(1)–N(1) and Al(1)–N(2) bond lengths (1.985(2) Å and 1.984(2) Å respectively in complex 4-Al compared to 2.079(3) Å and 2.064(3) Å in [AlH(BKIDip)2]).
This finding could potentially be a consequence of the extra oxygen atoms (O(2) and O(4)) within the enoate backbone of 4-Al. This may afford a resonance stabilization through inductive withdrawal of electron density from O(1) and O(3) respectively, causing a slight lengthening of the Al(1)–O(1) and Al(1)–O(3) bond lengths, concomitantly allowing the electron density of the N-groups to be more strongly donated to the Al center, resulting in slightly shorter Al–N bonds.
After the successful isolation of 4-Al, further attempts at synthesizing reactive gallium amidoenoate complexes were attempted. As hydride derivatives proved difficult to isolate previously, alkyl-substituents were targeted. By successfully obtaining [AlH(AMEDip)2] from an aluminium hydride adduct, we hypothesized that using a gallium alkyl species would provide a better route to the desired product, rather than trying to transform the chloride-substituent of complexes (1–3)-Ga to a methyl group. Scheme 4 shows the synthetic routes carried out towards the methyl gallium amidoenoate derivatives [GaMe2(AMEDip)] (4-Ga) and [GaMe2(AMEiPr)] (5-Ga). As neat trimethyl gallium is highly reactive, we employed the larger Dip-substituted aminoenoate pro-ligand in order to provide extra stabilization to the product formed. The 1:1 reaction of HAMEDip with [GaMe3] cooled to −78 °C in toluene was seen to evolve methane instantly upon addition. After allowing the reaction mixture to slowly warm to ambient temperature, all volatiles were removed yielding a viscous yellow oil. As tituration in hexane did not afford a solid, a range of NMR experiments and mass spectrometry confirmed that the oil was the pure 4-Ga (ESI†).
These included a singlet at δ = 0.04 ppm corresponding to the Ga(CH3)2 environment, a shift of 0.09 ppm when compared to free [GaMe3] (Ga(CH3)3 found at δ = −0.15 ppm) and two distinguished sets of doublets corresponding to ArCH(CH3)2 protons of the Dip-substituents at δ = 1.21 and 1.09 ppm with coupling values of 3JHH = 6.8 and 6.9 Hz respectively. The methine proton of the amidoenoate backbone was a singlet at δ = 4.90 ppm followed by the methine protons of the Dip-substituents (ArCH(CH3)2) at δ = 3.24 ppm.
The viscous nature of 4-Ga is proposed to be a consequence of the two remaining methyl groups bound to the gallium centre. Previous reports of methyl gallium derivatives also describe viscous products,28 however for solution-based applications such as AACVD, precursor viscosity does not present an issue. Following the successful isolation of 4-Ga, the smaller aminoenoate analogue (HAMEiPr) was employed in a similar reaction and afforded [GaMe2(AMEiPr)] (5-Ga) as a viscous pale oil. Multiple NMR experiments were again used to confirm that the oil was the pure complex [GaMe2(AMEiPr)] (ESI†). The peaks found included a singlet at δ = 0.11 ppm corresponding to the Ga(CH3)2 environment (downfield when compared to complex 4-Ga). A set of doublets corresponding to the isopropyl NCH(CH3)2 protons was observed at δ = 0.99 ppm (3JHH = 6.6 Hz) and overlapped with the terminal methyl group of the enoate tail (a triplet) at δ = 0.97 ppm (3JHH = 7.1 Hz). The methine proton of the amidoenoate backbone was a singlet at δ = 4.52 ppm, shifted up-field by 0.38 ppm when compared to complex 4-Ga. These differences suggest that the nature of the alkyl/aryl group at the N-position affects the acidity of the methine backbone proton in these complexes.
The chloride containing complex [AlCl(AMEDip)2] (3-Al) afforded ratios of Al2.2O2.9, whereas [AlH(AMEDip)2] (4-Al) resulted in the ratios of Al2.0O3.0. Similar results were observed for the gallium complexes with weight% ratios averaging 70:30 (Ga:O) for both complexes 1-Ga and 3-Ga, suggesting that film composition was not affected by the difference in steric bulk of these precursors. Furthermore, despite comparing the Cl-containing and Cl-absent precursors (3-Al and 4-Al respectively), X-ray photoelectron spectroscopy (XPS) survey analyses of all films suggested that no Cl was present in the deposited materials. This result implies that low atomic quantities of chlorine present in a precursor does not present a risk for chloride contamination during the AACVD process.
XPS analysis for films of α-Al2O3 deposited from 3-Al and 4-Al showed one distinct Al environment at an etch of 300 seconds. A representative example of XPS analysis from a film deposited from 3-Al is shown in Fig. 5.
Fig. 5 XPS analysis of an α-Al2O3 film deposited from complex 3-Al. Top: XPS of the Al 2p1/2 and 2p3/2 states. Bottom: XPS of the O 1s state. |
Peaks were found at 74.59 eV and 74.99 eV corresponding to the Al 2p3/2 and 2p1/2 environments respectively (separated by an energy gap of 0.40 eV) and with an intensity ratio of 1:2 (consistent with previously reported XPS analysis of Al3+).50–52 The O 1s binding energy was found at 531.39 eV and again confirmed the presence of an α-Al2O3 phase corresponding to the single environment observed. XPS analysis of thin films of β-Ga2O3 deposited from 1-Ga and 3-Ga showed the expected peaks for the Ga 2p1/2, Ga 2p3/2 as well as Ga 3d5/2 and 3d3/2 (ESI†) and were similar to previously reported gallium oxide XPS analyses.21,53
Scanning electron microscopy (SEM) was used to investigate the morphology of the deposited films, both on glass and quartz after annealing. Films deposited on glass with no annealing treatment showed a distribution of poorly connected, large particulates, consistent with the X-ray diffraction (XRD) patterns obtained for the samples deposited on glass, which were entirely amorphous and XRD patterns exhibited no conclusive information. Post-treatment annealing of the films was shown to improve the connectivity and definition of the surface particulates of all deposited material and improved the phase slightly as evidenced by XRD (ESI†). Example SEMs comparing the effects of annealing on films deposited from 3-Al are shown in Fig. 6. Similar SEMs were obtained for β-Ga2O3 deposited from 1-Ga and 3-Ga (ESI†).
Fig. 6 SEM images of the surface of a film deposited from 3-Al on glass (top) and on quartz after being annealed at 1000 °C for 12 hours in air (bottom). 1 μm scale bar inset. |
Ultraviolet–visible (UV-vis) spectroscopy was used to determine the transmittance of the films deposited on quartz. Table 3 shows the transmittance of the annealed thin films on quartz (ESI†). Transmittance measurements revealed that the annealed α-Al2O3 and β-Ga2O3 thin films transmitted 79–99% of visible light. Films deposited on glass were visibly coloured, however annealing the films on quartz afforded highly transparent and colourless films, which was reflected in the transmittance data.54,55
Precursor | Transmittance (%) |
---|---|
[GaCl2(AMEiPr)] (1-Ga) | 90 |
[GaCl(AMEDip)2] (3-Ga) | 79 |
[AlCl(AMEDip)2] (3-Al) | 95 |
[AlH(AMEDip)2] (4-Al) | 99 |
In most cases, the chlorido amidoenoate complexes were extremely stable to a variety of transformation reactions, such as hydride sources (including alkali metal hydride salts, alkyl silanes and magnesium hydride dimers) which were used in attempts to transform the {M–Cl} moiety to {M–H}. However, by varying the group 13 source, different functionalities could be installed as evidenced by the synthesis of amidoenoate complexes exhibiting {Al–H} (4-Al) and {Ga–C} (4-Ga and 5-Ga) bonds.
A proof-of-concept study using a selection of these complexes (1-Ga, 3-Ga, 3-Al and 4-Al) in AACVD experiments was carried out. These initial studies present the precursors as suitable options for routes to the deposition of the corresponding group 13 oxide. Standard deposition conditions for the films included a deposition temperature of 500 °C from toluene mixtures of the precursors, which deposited the expected amorphous material on glass. Subsequent annealing of the material on quartz substrates at 1000 °C in air for 12 hours afforded more crystalline oxide material. The films deposited were analysed using standard techniques (XRD, XPS, EDAX, SEM and UV-Vis) and confirmed the composition of the α-Al2O3 and β-Ga2O3 films, their elemental stoichiometry, transparency, and morphological characteristics. The geometries of the complexes, quantified using the τ-parameter, provide an indication of the precursors potential deposition profile. This shows that, at least for the system of the group 13 oxides Al2O3 and Ga2O3, precursors that are not sterically strained (τ-value closer to 0 or 1) afford materials that exhibit improved transmittances after deposition. In-depth AACVD investigations related to these systems are currently underway.
Single crystal X-ray diffraction (XRD) data were collected using a SuperNova Atlas (Dual) diffractometer using Cu Kα1 radiation of wavelength 1.54184 Å. Suitable crystals were selected and mounted on a nylon loop and the crystal kept at 150 K during data collection. Using Olex2,57 we solved the structure with the olex2.solve58 structure solution program using Charge Flipping and refined with the ShelXL59 refinement package using Least Squares minimization. Nuclear magnetic resonance (NMR) data were recorded in either CDCl3 or C6D6 (obtained from Sigma, dried on sieves and stored under an inert atmosphere) using a Bruker Avance 300, Bruker Avance Neo 500 or Bruker Avance Neo 700 MHz instrument at ambient temperature. 1H and 13C{1H} NMR assignments were confirmed by 1H–1H (COSY and NOESY) and 1H–13C (HSQC and HMBC) experiments where necessary. Mass spectra were obtained using a Micromass 70-SE spectrometer using electrospray chemical ionization in the positive mode (ESI+). XRD for thin films was carried out with a Bruker D8 Discover X-ray diffractometer using monochromatic Cu Kα1 and Cu Kα2 radiation of wavelengths 1.54056 and 1.54439 Å, respectively, emitted in an intensity ratio of 2:1, voltage = 40 kV; current = 40 mA. SEM/EDXA was performed using a Philips XL30 FEG with an electron beam accelerating energy of 30 kV. XPS profiling was performed using a Thermo Scientific K-Alpha XPS system using monochromatic Al Kα radiation at 1486.6 eV X-ray source. CasaXPS software was used to analyse the binding energy of the data, referenced to a C 1s peak at 284.8 eV. UV/vis/NIR transmission spectra were recorded using a PerkinElmer Lambda 950 spectrometer in the range of 300–1400 nm with a background of air, and Tauc plots from this data were used to calculate the band gaps.
Depositions were carried out under argon (99.99% from BOC). The synthesized precursors were placed into an inert AACVD glass bubbler and dissolved in an appropriate dry solvent. Two glass substrates were placed into a horizontal bed cold-wall reactor chamber, one resting on top of the graphite heating block, the second resting 0.5 cm above, ensuring a laminar flow of gas. The glass substrates were cleaned prior to deposition with isopropyl alcohol, water, and acetone and allowed to dry in air before the deposition took place. The temperature of the graphite block was controlled with a thermocouple composed of platinum-rhodium rods. An ultrasonic nebulizer containing a piezoelectric device (functioning at 20 kHz) was used to generate an aerosol mist of the precursor. The mist was carried into the reaction chamber via a flow of ultra-pure argon gas, which was optimized at a flow rate of 1 L min−1.
Footnote |
† Electronic supplementary information (ESI) available: Homonuclear and heteronuclear NMR data, X-ray crystallography collection data and XPS, SEM and UV-Vis data. CCDC 2101966, 2101967, 2101971, 2101972, 2101973, 2101974 and 2101975. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/d1dt03365d |
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