Sixberth
Mlowe
a,
David J.
Lewis
b,
Mohammad Azad
Malik
ab,
James
Raftery
b,
Egid B.
Mubofu
c,
Paul
O'Brien
b and
Neerish
Revaprasadu
*a
aDepartment of Chemistry, University of Zululand, Private Bag X1001, KwaDlangezwa, 3886, South Africa. E-mail: RevaprasaduN@unizulu.ac.za
bSchools of Chemistry and Materials, The University of Manchester, Oxford Road, Manchester, M13 9PL, UK
cDepartment of Chemistry, University of Dar es Salaam, P.O. Box 35061, Dar es Salaam, Tanzania
First published on 18th December 2015
Tris-(piperidinedithiocarbamato)iron(III) (1) and tris-(tetrahydroquinolinedithiocarbamato)iron(III) (2) complexes have been synthesized and their single-crystal X-ray structures were determined. Thermogravimetric analysis (TGA) of the complexes showed decomposition to iron sulfide. Both complexes were then used as single-source precursors for the deposition of iron sulfide thin films by aerosol-assisted chemical vapour deposition (AACVD). Energy-dispersive X-ray (EDX) spectroscopy confirmed the formation of iron sulfide films. The addition of tert-butyl thiol almost doubled the sulfur content in the deposited films. Scanning electron microscopy (SEM) images of the iron sulfide films from both complexes showed flakes/leaves/sheets, spherical granules and nanofibres. The sizes and shapes of these crystallites depended on the nature of the precursor, temperature, solvent and the amount of tert-butyl thiol used. The observed optical properties are dependent upon the variation of reaction parameters such as temperature and solvent. Powder X-ray diffraction (p-XRD) studies revealed that pyrrhotite, hexagonal (Fe0.975S), marcasite and smythite (Fe3S4) phases were differently deposited.
Iron sulfide compounds exhibit a wide range of properties, from the semiconducting FeS2 to ferromagnetic Fe3S4.13 In contrast to the properties of their bulk counterparts, iron sulfide thin films and nanoparticles can exist in magnetic structures with enhanced surface contributions. Amongst the iron sulfide phases, cubic-FeS2 (pyrite) has attracted most interest, in particular in the development of thin-film solar cells and solid-state batteries, owing to its properties which include strong light absorption (∼5 × 105 cm−1) and a direct band gap of 0.95 eV.14–17
Several studies on the deposition of iron sulfide thin films using single source precursors have been reported.18–20 Aerosol-assisted chemical vapour deposition (AACVD) is a versatile route for the deposition of iron sulfide thin films. The morphology, particle size and crystal-structure of the films deposited by this route can be closely controlled by the choice of a suitable solvent, deposition temperature and the nature of the precursor. We have been using single source precursors for metal chalcogenide thin films or nanoparticles and recently used complexes such as dithiocarbamates,21–24 thiosemicarbazone25 and thiobiurets26 for the preparation of Fe–S thin films by AACVD.
Herein we report the synthesis and X-ray crystal structures of new iron(III) dithiocarbamate complexes, tris-(piperidinedithiocarbamato)iron(III) (1) and tris-(tetrahydroquinolinedithiocarbamato)iron(III) (2). These complexes have been used as single-source precursors for the deposition of iron sulfide thin films by AACVD. Powder X-ray diffraction, scanning electron microscopy and optical measurements reveal that the structural and electronic properties of the as-prepared nanostructured iron sulfide films are strongly dependent on sample preparation conditions such as temperature and solvent effects. The effect of temperature and solvent also played an important role in controlling the surface morphology and phase chemistry of the deposited films. Structural and morphological transformations in the deposited films were also observed as a result of the change in the chemical structure of the starting materials, allowing the fabrication of rare phases of iron sulfide that have not been accessed before by AACVD. The decomposition mechanism of complex (1) is also proposed, based upon thermal analysis, gas chromatography mass spectroscopy (GC MS) and powder X-ray diffraction studies.
Single crystal X-ray diffraction data for the compounds were collected using graphite monochromated Cu-Kα radiation (λ = 1.54178 Å) on a Bruker APEX diffractometer. The structure was solved by direct methods and refined by full-matrix least squares on F2. All non-H-atoms were refined anisotropically. Hydrogen atoms were included in calculated positions, assigned isotropic thermal parameters and allowed to ride on their parent carbon atoms. All calculations were carried out using the SHELXTL software package.27 The crystallographic refinement parameters are detailed as follows:
X-ray experimental and structural refinement data for C18H30FeN3S6 (1) (Fig. 2). C18H30FeN3S6, M = 536.66, monoclinic, space group C2/c, a = 13.0387(9), b = 11.8818(9), c = 15.9260(15) Å, α (°) = 90, β (°) = 101.292(6), γ (°) = 90, volume = 2419.5(3) Å3, Z = 4, D = 1.473 Mg m−3, T = 100(2) K, reflections collected = 8309/2300, unique reflections = [R(int) = 0.0695], final R indices [I > 2σ(I)]R1 = 0.0541, wR2 = 0.1176, R indices (all data) R1 = 0.0707, wR2 = 0.1336, largest diff. peak and hole = 0.707 and −0.935 e Å−3, GOF = 1.068. CCDC reference number 984433.
X-ray experimental and structural refinement data for C30H30Fe1N3S6 (2) (Fig. 3). C30H30Fe1N3S6, M = 680.78, orthorhombic, space group Pca2(1), a = 21.9551(8), b = 18.8423(6), c = 14.7741(4) Å, α (°) = 90, β (°) = 90, γ (°) = 90, volume = 6111.8(3) Å3, Z = 4, D = 1.480 Mg m−3, T = 100(2) K, reflections collected = 24173/8695, unique reflections = [R(int) = 0.0991], final R indices [I > 2σ(I)]R1 = 0.0670, wR2 = 0.1576, R indices (all data) R1 = 0.1083, wR2 = 0.1784, largest diff. peak and hole = 1.034 and −0.614 e Å−3, GOF = 1.027. CCDC reference number 1008838.
To an aqueous solution of FeCl3 (0.82 g, 5.0 mmol) (25 mL) was added dropwise an aqueous solution of the ligand, NaC10NS2H10 (3.482 g, 15.0 mmol), dissolved in a minimal amount of water, with vigorous stirring. The reaction mixture was stirred for a further 1 h before being filtered. The black-coloured solids were washed with deionized water and dried under vacuum overnight. The compound was found to be soluble in solvents such as chloroform and dichloromethane and solubility in toluene is enhanced at elevated temperatures. The complexes were recrystallized from chloroform and hexane (1:
1) by the diffusion method, to obtain crystals of complex (1) C18H30FeN3S6. Complex (2) C30H30FeN3S6 was prepared in a similar manner.
Yield 79.7%. Elemental analysis for C18H30FeN3S6: Calc: C, 40.28; H, 5.63; N, 7.83; S, 35.85; Fe, 10.41. Found: C, 40.32; H, 5.73; N, 7.94; S, 35.34; Fe, 9.55. IR (cm−1): 1422 (CN), 965 (C
S), 365 (Fe–S).
Yield 62.4%. Elemental analysis for C30H30FeN3S6: Calc: C, 52.93; H, 4.54; N, 6.17; S, 28.26; Fe, 8.20. Found: C, 53.19; H, 4.99; N, 6.42; S, 27.76; Fe, 7.81. IR (cm−1): 1440 (CN), 978 (C
S), 383 (Fe–S).
Precursor | Reaction conditions | Morphology | Phase |
---|---|---|---|
Complex (1) | Toluene, 350–450 °C, 2 h | Leaf, flake, sheet | Hexagonal (Fe0.975S), marcasite (FeS2) |
Chloroform, 350–450 °C, 30 minutes | Fiber | Hexagonal (Fe0.975S), smythite (Fe3S4) | |
tert-Butyl thiol, 450 °C, 2 h | Flower, spherical-globular | Greigite (Fe3S4) | |
Complex (2) | Toluene, 350–450 °C, 2 h | Leaf, flake, sheet | Pyrrhotite (Fe0.95S1.05), hexagonal (Fe0.975S) |
Chloroform, 350–450 °C, 30 minutes | Fiber | Hexagonal (Fe0.975S) | |
tert-Butyl thiol, 450 °C, 2 h | Spherical and flake | Greigite (Fe3S4) |
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Fig. 1 (a) The X-ray single crystal structure of C18H30FeN3S6 (CCDC 984433) (red = Fe, yellow = S, blue = N and black = C). Selected bond lengths (Å) and bond angles (°): Fe(1)–S(1) 2.2920 (13), Fe(1)–S(1) #1 2.2920 (13), Fe(1)–S(3) #1 2.3003 (13), Fe(1)–S(3) 2.3003 (13), Fe(1)–S(2) 2.3067 (13), Fe(1)–S(2) #1 2.3067 (13), S(1)–Fe(1)–S(1) #1 99.40 (7), S(1)–Fe(1)–S(3) #1 93.87 (4), S(1) #1–Fe(1)–S(3) #1 162.84 (5), S(1)–Fe(1)–S(3) 162.84 (5), S(1) #1–Fe(1)–S(3) 93.88 (4), S(3) #1–Fe(1)–S(3) 75.46 (6), S(1)–Fe(1)–S(2) 75.81 (5), S(1) #1–Fe(1)–S(2) 94.62 (5), S(3) #1–Fe(1)–S(2) 99.17 (5), S(3)–Fe(1)–S(2) 92.41 (5), S(1)–Fe(1)–S(2) #1 94.62 (5), S(1) #1–Fe(1)–S(2) #1 75.81 (5), S(3) #1–Fe(1)–S(2) #1 92.41 (5), S(3)–Fe(1)–S(2) #1 99.17 (5), S(2)–Fe(1)–S(2) #1 165.37 (8). (b) The X–ray single crystal structure of C30H30FeN3S6 (CCDC 1008838) (red = Fe, yellow = S, blue = N and black = C). Selected bond lengths (Å) and bond angles (°): Fe(1)–S(6) 2.293 (3), Fe(1)–S(2) 2.299 (3), Fe(1)–S(3) 2.307 (3), Fe(1)–S(5) 2.308 (3), Fe(1)–S(4) 2.309 (3), Fe(1)–S(1) 2.316 (3), S(6)–Fe(1)–S(2) 95.56 (11), S(6)–Fe(1)–S(3) 163.17 (12), S(2)–Fe(1)–S(3) 96.38 (11), S(6)–Fe(1)–S(5) 75.86 (10), S(2)–Fe(1)–S(5) 163.44 (12), S(3)–Fe(1)–S(5) 95.21 (11), S(6)–Fe(1)–S(4) 91.27 (11), S(2)–Fe(1)–S(4) 95.70 (11), S(3)–Fe(1)–S(4) 75.78 (10), S(5)–Fe(1)–S(4) 98.59 (10), S(6)–Fe(1)–S(1) 99.53 (11), S(2)–Fe(1)–S(1) 75.20 (10), S(3)–Fe(1)–S(1) 94.97 (11), S(5)–Fe(1)–S(1) 92.06 (10), S(4)–Fe(1)–S(1) 166.42 (12). |
The single crystal X-ray structure of tris-(tetrahydroisoquinolinedithiocarbamato)iron(III) (2) is shown in Fig. 1(b). The structure also shows a distorted octahedral environment with the Fe–S distances between 2.293 and 2.316 Å, longer than those of complex (1). The Fe–S bond lengths from both complexes (1) and (2) are closer to those observed in our previous work.29 The bite angles 75.20°, 75.78° and 75.86° of S1–Fe1–S2, S3–Fe1–S4 and S5–Fe1–S6, respectively, further reveal the distorted octahedral geometry on iron(III). Structural refinement data are given in the Experimental section; selected bond angles and lengths are presented in the caption to Fig. 1(b).
Thermogravimetric analysis (TGA) of complex (1) showed a two-step decomposition pattern with a rapid weight loss of 15.6% and 65.5% at 210 °C and 304 °C, respectively (Fig. 2). The weight of the remaining residue is 15.7%, which corresponds to FeS (calculated percentage 16.4%). The thermogram of complex (2) shows an ill-defined three-step decomposition pattern with a weight loss of 28.0%, 44.3% and 7.1% at 207 °C, 257 °C and 351 °C, respectively; the final weight of 11.8% (calculated 12.9%) is assumed to be a residue of the iron sulfide material, which is sulfur deficient (Fig. 2). The thermogram of complex (2) seems to continue changing on approaching 700 °C, possibly due to residual carbonaceous species in the films, or sublimation of the iron sulfide product, perhaps leading to sulfur deficient phases. Another possibility is that oxide phases form; Fe is very oxophilic and the nitrogen in the TGA is probably not that dry or oxygen free.
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Fig. 2 Thermogravimetric analysis (TGA) of complexes (1) and (2) at a heating rate of 10 °C min−1 under nitrogen with a flow rate of 10 cm3 min−1. |
The decomposition mechanism of complex (1) was investigated using thermogravimetric analysis (TGA), gas chromatography mass spectroscopy (GC/MS) and powder X-ray diffraction (p-XRD). Thermal studies show that the decomposition of the complex (1) proceeds through two major steps: (i) detachment of one of the three dithiocarbamate ligands in the six coordinated tris-(piperidinedithiocarbamato)iron(III) complex, thus forming an intermediate four coordinated complex, and lastly (ii) the final decomposition/elimination (304 °C) of the four coordinated dithiocarbamato complex of iron to afford materials of either FeS or indefinite Fe–S composition (Fig. 3). The first weight loss of 15.6% is smaller than the weight of the anticipated release of only one piperidine dithiocarbamate ligand (∼29%). Thus, the first step may involve partial decomposition, rearrangement of the complex and/or reduction to a Fe(II) complex. The GC mass spectrum of complex (1) also confirmed complete decomposition of the complex via two steps (ESI Fig. 1†): (i) elimination of one piperidinyl dithiocarbamato ligand (m/z 160), followed by (ii) complete removal of the remaining organic components (m/z 290), thus affording FeS as the final product (m/z 86).
A separate study which aimed at identifying the existence of temperature-dependent phase transformation in the iron sulfide materials was carried out. The progress of this experiment was monitored using powder X-ray diffractometry. Diffraction studies (ESI Fig. 2†) were carried out at a heating rate of 2.5 °C h−1, where complex (1) was the starting material heated from 180 °C to 310 °C under N2 flow. A total of 27 diffraction patterns were collected. The hexagonal phase (card number 01-080-1032) of iron sulfide and mackinawite (card number 04-003-6935) became prominent with an increase in temperature, with few peaks unassigned. The observed temperatures for the occurrence of Fe–S phases are lower than those established from phase diagrams, probably due to the prolonged time of the diffraction analysis and heating.
The SEM images of iron sulfide films in Fig. 4 deposited using complex (1) in toluene solvent show the growth of sheet-like structures at 350 °C and nano-leaf/flake like crystallites at 400 °C and 450 °C. The film size increased with an increase in deposition temperature; an increase in film size of 0.6–1.0 μm was observed when the temperature was increased to 400 °C and 450 °C. Some microstructures on the surfaces were also observed. The morphology obtained from this study is reasonably similar to that of our recently reported iron sulfide thin films deposited using iron thiobiuret and diethyldithiocarbamate complexes.21,27 EDX spectroscopy on five different areas of the films showed that the compositions are slightly sulfur deficient, a trend that increased at an elevated temperature (Table 2).
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Fig. 4 Representative secondary electron SEM images of the iron sulfide thin films deposited at (a and b) 350 °C, 400 °C (c and d) and (e and f) 450 °C using complex (1). |
Temp (°C) | Fe (%) | S (%) | Ratio (Fe![]() ![]() |
---|---|---|---|
350 | 57.3 | 42.7 | Fe(1+x)S, x = 0.3 |
400 | 60.8 | 39.2 | Fe(1+x)S, x = 0.5 |
450 | 66.3 | 33.7 | Fe2S |
A similar trend was observed when complex (2) was used as the single source precursor to deposit a pyrrhotite film (Fig. 5a and b). The images illustrate the formation of typical nanosheet-like structures. A slight morphological transformation is observed, as a result of the change in the chemical structure of the starting materials.
The back-scattered electron (BSE) SEM image (which provide Z contrast) of iron sulfide films shows small particles with bright contrast embedded into flakes of darker contrast. Point scanning EDX spectroscopy revealed that the white spots (chunks) were S-rich (Fe 53.7% and S 46.3%), while the opposite is observed for the black spots (flakes) which are Fe-rich (Fe 66.9% and S 33.1%) (Fig. 5c). This phenomenon validates that Fe and S atoms in an iron sulfide thin film are unevenly distributed on a substrate, strongly suggestive of the formation of an overall S-deficient film. The darkness of the iron rich area suggests that there is a lighter element such as carbon in this area of the film that tends to darken the contrast compared to the small crystallites observed which appear white.
The p-XRD patterns of the as-deposited films from complex (1) show hexagonal-phase iron sulfide (Fe0.975S) (card number: 01-080-1032), dominating at the higher temperature of 450 °C (Fig. 6(a)). The reflection (hkl) planes of (110), (201) (114) (214) and (220) corresponding to the Fe0.975S phase were observed at 450 °C. At the deposition temperatures of 350 °C and 400 °C, the XRD patterns showed mixed phases of marcasite (FeS2) and iron sulfide (Fe0.975S) phases. The reflections at 25.97°, 37.38°, 38.89° and 40.59° were indexed to the (110), (111), (120) and (200) planes of marcasite FeS2 (card number: 03-065-2567). Mixed phases of marcasite (FeS2) and hexagonal iron sulfide (Fe0.975S) coexist at 350 °C and 400 °C, while the latter are predominantly obtained in its pure phase at 450 °C. The transformation of iron sulfide compounds into different phases is possible under certain conditions such as high temperature or pressure.30–32
A comparison of p-XRD patterns for the iron sulfide film deposited from complex (2) by AACVD at 350, 400 and 450 °C is presented in Fig. 6(b). A pure hexagonal-pyrrhotite 1 T (Fe0.95S1.05) phase is formed at 450 °C (card number: 01-075-0600), while at 350 and 400 °C some additional peaks are observed (denoted by the symbol #) which matched a hexagonal iron sulfide phase (Fe0.975S) (card number 01-080-1032). These results suggest that the mechanism by which the complexes decompose are different. Intergrowth involving different pyrrhotite types is known,33–35 and the degree of such intergrowths (micron to submicron) makes analysis difficult and therefore information on accurate Fe:
S ratios and the concentration of impurity is relatively incomplete for the pyrrhotite in this study. These results are similar to our recent reports,21,22 where formation of the pyrrhotite phase was observed at 400 and 450 °C when alkyldithiocarbamatoiron(III) complexes were used as single source precursors to deposit films by AACVD.
The UV-vis NIR absorption spectrum of the iron sulfide thin film deposited at 350, 400 and 450 °C is shown in Fig. 7. The as-deposited iron sulfide thin films absorb light in the visible and near-infrared spectral regions. Deposition from complex (1) at 350 °C displays a sharp absorption band gap of 1.63 eV, estimated from Tauc plots (inset, Fig. 7).36 The films deposited at 400 and 450 °C exhibited red shifted absorption properties (∼1.25–1.34 eV) compared to those of 350 °C. The blue shift observed for the absorption spectra may reveal the formation of surface defects free37 and hence high optical performance activeness of the films in the visible and infrared region. The optical behaviour of the deposited films reveals that the absorption properties are temperature, size and structure dependent.
The p-XRD patterns of iron sulfide films grown from chloroform solutions of complex (1) at all temperatures (Fig. 9(a)) showed (112), (201), (203), (320), (220) and (222) reflections which correspond to hexagonal-phase iron sulfide (Fe0.975S) (card number: 01-080-1032). Some minor peaks can be attributed to the smythite phase (Fe3S4) (card number 04-007-2189) are observed at 350 °C, while a pure hexagonal phase is observed at temperatures 400 °C and 450 °C. Furthermore, the intensity of the (112) reflection increases as a function of temperature. The growth of a hexagonal phase-iron sulfide (Fe0.975S) from complex (2) dominates at all deposition temperatures (Fig. 9(b)). UV-Vis-NIR absorbance spectroscopy of a representative sample (350 °C for complex (1)) showed a broad absorption with the absorption maxima at around 1300 nm (0.95 eV) at 350 °C (ESI Fig. 3†), bathochromically shifted compared with films produced using toluene solvent. These results reveal that the solvent plays an important role in the reaction pathway.
Addition of t-BuSH to the precursor mix had a strong influence on the morphologies of the deposited iron sulfide films. SEM images (Fig. 10a and b) of iron sulfide films deposited using complex (1) at 450 °C showed the formation of flower-like bundles of spherical-to-globular shaped crystallites with particle sizes ranging from 500 to 600 nm. Complex (2) deposited double-layered films: the bottom one, a relatively compact layer, is composed of spherical particles (∼500 nm), and a loose top layer is composed of mainly flake shaped crystallites (900 nm) (Fig. 10c and d). A significant increase in the sulfur content (S 53.8% and Fe 46.2%) was observed as a result of using t-BuSH. The p-XRD patterns of deposited iron sulfide samples reveal two sharp reflections at 32° and 45.8° which we could not assign (ESI Fig. S4†).
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Fig. 10 SEM images of the iron sulfide thin films deposited at 450 °C using (a and b) complex (1) and (c and d) complex (2). |
Topological analysis of the films was performed using atomic force microscopy (AFM), and revealed the formation of uniform films (ESI Fig. S5†). The room temperature UV-Vis NIR absorption spectra, shown in ESI (Fig. S6†), of iron sulfide thin films deposited using complexes (1) and (2) both showed an absorption edge of approx. 1.7–2.0 eV, a hypsochromic shift compared with the reported values of iron sulfide.40,41 This blue shift phenomenon confirms the enrichment of the Fe–S film by sulfur, as a result of t-BuSH addition. It has been reported that sulfur vacancies and impurities are potentially responsible for lowering the band gap of iron sulfide particles.37,42 Additionally, bulk sulfur vacancies are also responsible for nonconstant charge distribution, resulting in poor optical properties and photoconversion efficiency.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 984433 and 1008838. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c5dt03881b |
This journal is © The Royal Society of Chemistry 2016 |