Sixberth
Mlowe
ab,
David J.
Lewis
b,
M.
Azad Malik
b,
James
Raftery
b,
Egid B.
Mubofu
c,
Paul
O'Brien
b and
Neerish
Revaprasadu
*a
aDepartment of Chemistry, University of Zululand, Private Bag X1001, Kwa-Dlangezwa, 3886, South Africa. E-mail: RevaprasaduN@unizulu.ac.za; Fax: +27 35 902 6568; Tel: +27 35 902 6152
bSchools of Chemistry and Materials Science, 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 19th September 2014
The synthesis and single-crystal X-ray structure of bis(piperidinedithiocarbamato)pyridinecadmium(II), [Cd(S2C(NC5H10))2(NC5H5)] are reported and its use as a precursor for the synthesis of hexagonal CdS nanoparticles and CdS thin films is presented. Thermogravimetric analysis (TGA) of this complex showed clean decomposition in two steps to give CdS. Thermolysis of the complex in hexadecylamine at different temperatures in the range 190–270 °C gave CdS nanostructures including nanorods and oval shaped particles. The band gap of the as-synthesized CdS nanoparticles varied as the temperature was increased. CdS thin films with optical direct band gaps of ca. 2.4 eV were deposited by aerosol-assisted chemical vapour deposition (AACVD) in the temperature range 350 to 450 °C using the same precursor. Powder X-ray diffraction (p-XRD) patterns of CdS nanoparticles and thin films confirmed the hexagonal phase of CdS.
Indeed, the physical properties and single crystal X-ray structural studies on numerous cadmium and zinc complexes comprising dithiocarbamate and aromatic nitrogen-containing chelating ligands such as pyridine, 2,2′-bipyridine and 1,10-phenanthroline have been reported.14–17 These five and six coordinate complexes showed increased electron density at the metal centre. Thermal properties of these adducts include increased volatility upon introduction of the Lewis base ligands containing nitrogen.18 Studies on the effect of pyridine and other nitrogen donor ligands in heterocyclic cadmium dithiocarbamate complexes on properties of CdS nanoparticles have recently been reported. Srinivasan and Thirumaran have investigated the influence of pyridine as a ligand in the precursor for the synthesis of CdS nanoparticles.19 Onwudiwe et al. synthesized CdS nanoparticles by thermolysis of the 2,2′-bipyridine and 1,10-phenanthroline adduct of cadmium ethyl phenyl dithiocarbamate complexes in hexadecylamine (HDA).20 In both studies, the incorporation of nitrogen-donor ligands in the precursor enhances the axial growth direction of CdS nanoparticles.21
Various single-source precursors have been used for the preparation of CdS thin films deposition by a number of chemical vapour deposition (CVD) methods.22–25 O'Brien and co-workers have reported a number of dithiocarbamatocadmium(II) complexes as single source precursors for CdS thin films using low pressure metal–organic chemical vapour deposition (LP-MOCVD).18,26 Aerosol-assisted chemical vapour deposition (AACVD) has been used to deposit a wide range of metal chalcogenide thin films.27–29 Several adducts of cadmium dithiocarbamate complexes have recently been reported but without exploring their capabilities as precursors for AACVD.15–17 Ehsan et al. used bis(N,N-dicyclohexyldithiocarbamato)pyridinecadmium(II) to deposit greenockite CdS thin films which proved to be suitable for application in photoelectrochemical (PEC) cells.30 CdS thin films possess good electrical and optical properties, including wide band gaps (ca. 2.4 eV) making it an ideal material for solar cell device fabrication.31
Herein, we report the synthesis and single crystal X-ray structure of the pyridine adduct of bis(piperidinedithiocarbamato)cadmium(II) and we evaluate its potential as a single-source precursor for the deposition of hexagonal CdS thin films and nanoparticles.
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 package. The crystallographic refinement parameters are detailed in the next paragraph.
X-ray experimental and structural refinement data for [Cd(S2C(NC5H10))2(NC5H5)] (Fig. 1): C17H25CdN3S4, M = 512.04, monoclinic, space group P2(1)/c, a = 8.8114(4), b = 9.8021(5), c = 24.4201(11) Å, α (°) = 90, β (°) = 95.928(2), γ (°) = 90, volume = 2097.89(17) Å3, Z = 4, D = 1.621 mg m−3, T = 180(2) K, reflections collected = 10171/3882, unique reflections = [R(int) = 0.0534], final R indices [I > 2σ(I)]R1 = 0.0349, wR2 = 0.0870, R indices (all data) = R1 = 0.0365, wR2 = 0.0882, largest diff. peak and hole = 0.830 and −0.571 e Å3, GOF = 1.048. CCDC 984434.
NaS2C(NC5H10), yield: 16.4 g (90%). 1H NMR (400 MHz, D2O): σ 1.41 (m, 2H, 3-CH2), 1.53 (t, 2H, 4-CH2), 4.28 (t, 2H, 2-CH2). IR (νmax in cm−1, ATR): 967, ν(CS); 1468, ν(C
N). Anal. calc. for C6H12NS2ONa (%): C, 35.8; H, 6.01; N, 6.96. Found (%): C, 35.9; H, 6.13; N, 6.98.
[Cd(S2C(NC5H10))2], yield: 1.71 g (79%). 1H NMR δ ppm (400 MHz, DMSO): 4.13 (t, 8H, 2-CH2), 1.73 (t, 4H, 3-CH2),1.63 (m, 8H, 3-CH2), IR (νmax in cm−1, ATR): 967, ν(CS); 1485, ν(C
N); 388, ν(Cd–S). Anal. calc. for C12H20N2S4Cd (%): C, 33.29; H, 4.66; N, 6.47. Found (%): C, 33.47; H, 4.55; N, 6.43.
[Cd(S2C(NC5H10))2(NC5H5)], yield: 0.61 g (97%). IR (νmax in cm−1, ATR): 989, ν(CS); 1544, ν(C
N); 402, ν(Cd–S). Anal. calc. for C17H25N3S4Cd (%): C, 39.87; H, 4.92; N, 8.21. Found (%): C, 39.08; H, 4.32; N, 7.69.
The single crystal X-ray structure of bis(piperidinedithiocarbamato)pyridinecadmium(II) [Cd(S2C(NC5H10))(NC5H5)], is shown in Fig. 1. There are three coordinating ligands of two different molecules in the symmetric unit of the complex. Coordination to the central Cd(II) metal is characterised by 4 × S and 1 × N bonds from two piperidine dithiocarbamate (bidentate) and pyridine ligands, respectively forming a five coordinated complex. The geometry of the complex is a square pyramidal. The bond lengths of Cd–S range from 2.5648 to 2.6684 Å, which are longer than that of Cd–N (2.320 Å) as expected. Two of the Cd–S bond lengths are relatively longer than the other two in each dithiocarbamato ligand as observed previously.32 Structural refinement data are given in the experimental; selected bond angles and lengths are presented in the caption to Fig. 1.
Thermogravimetric analysis (TGA) gives insight into the decomposition of precursors and what products might be expected. TGA of the pyridine adduct of bis(piperidine dithiocarbamato)cadmium(II) complex reveal a two-step decomposition with weight loss between ca. 130 and 320 °C (Fig. 2). The solid decomposition residue amounts to 31% for the pyridine adduct which is close to the calculated value of 28% for CdS for this complex. Previous studies on the cadmium piperidine dithiocarbamate complexes had steep one-step decomposition with a rapid weight loss at 329 °C, mirrored in the second decomposition step of the pyridine adduct.10 In the case of the adduct, the first decomposition temperature is due to the loss of the pyridine ligand, confirmed by the percentage loss of 14.1% from the TGA plot.
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Fig. 2 Thermogravimetric analysis (TGA) plot of the pyridine adduct [Cd(S2C(NC5H10))2(NC5H5)] at a heating rate of 10 °C min−1 under a nitrogen atmosphere. |
CdS nanoparticles were synthesis from the thermolysis of [Cd(S2C(NC5H10))2(NC5H5)] in hexadecylamine at various temperatures, and their optical properties were tested. Usually, two photoluminescence (PL) emission peaks can be observed from semiconductor nanoparticles. The first is excitonic emission which is sharp and located near the absorption edge of the particle and a second deep trap emission which is broad and Stokes shifted compared to the excitonic emission.33,34 The UV-vis absorption spectrum for CdS nanoparticles synthesized at 190 °C reveal a sharp absorption band edge at 468 nm (Fig. 3(A)). The corresponding PL spectrum displays a narrow band edge emission, with a maximum at 478 nm (Fig. 3(A)). The bathochromic shift observed is typical for nanostructured semiconductors.35,36 There is also a weaker broad emission observed in the 560–670 nm regions which is most likely due to electron–hole recombination from surface defects. The Stokes shift observed is typical for nanostructured semiconductors.35,36
The effect of reaction temperature on the optical absorption of CdS nanoparticles has been investigated. The absorption spectra for CdS nanoparticles synthesized at 190, 230 and 270 °C are shown in Fig. 3(B). The well-defined absorption band edge at 468 nm observed for the CdS synthesized at 190 °C is less prominent for the samples synthesized at 230 and 270 °C. The band edge for CdS nanoparticles synthesised at 230 °C is observed at 479 nm, while the band edge of CdS nanoparticles synthesised at 270 °C is further red-shifted to 496 nm. Reaction time produced negligible effects in the optical spectra; samples were collected after 1 and 2 hours with little changes in the absorption and emission spectra. The formation of CdS nanocrystals was also monitored with UV-vis absorption spectroscopy. As nanoparticles grow in size, the bandgap absorption edge is bathochromically shifted. Upon increase of the reaction temperature from 190 °C to 270 °C, the growth rate of the CdS nanocrystals is increased. A potential reason for this phenomenon could be that higher reaction temperature results in the formation of irregular nanoparticles with reduced crystallinity due to random, faster nucleation and with the rapid growth affecting the ligand configuration at the nanocrystal surface.37
TEM and HRTEM images of the CdS nanoparticles synthesised from [Cd(S2C(NC5H10))2(NC5H5)] at 190, 230 and 270 °C are shown in Fig. 4(a)–(f). The CdS nanoparticles obtained at low temperature (190 °C) are rod shaped (Fig. 4(a)) with a length of 64.38 ± 4.62 nm, a width of 5.20 ± 0.98 nm and an aspect ratio of 12.38. Similar morphologies were obtained using [Cd(S2CNC5H10)2] as a precursor whereby multiple-armed rods of CdS were obtained.9–11 When the reaction temperature was increased to 230 °C (Fig. 4(c)), rods with a reduced average length of 24.84 ± 4.42 nm and breadth of 6.58 ± 1.02 nm were obtained. The corresponding HRTEM images (Fig. 4(b) and (d)) show particles with lattice fringes. The particles synthesized at 230 °C have lattice fringes with a d-spacing of 3.15 Å corresponding to the (002) plane of hexagonal CdS. At 270 °C, the shape of the CdS nanoparticles evolved from rod to an oval shaped morphology with diameters ranging from 16.8 to 23.3 nm (Fig. 4(f)); the aspect ratio of the nanorods decreased with the increase in temperature.37 The oval shape of the particles was confirmed by the HRTEM image (Fig. 4(f)). The lattice fringes have a d-spacing of 3.13 Å corresponding to the (002) basal plane of hexagonal CdS. In summary, CdS nanoparticles synthesized at higher temperature, favour the thermodynamic growth regime resulting in isotropic particles (spherical and cubes) while CdS nanoparticles synthesised at lower temperatures favour non-equilibrium kinetic growth regime and yields anisotropic particles (rods).38
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Fig. 4 TEM and HRTEM images of HDA capped CdS nanoparticles synthesized by thermolysis of [Cd(S2C(NC5H10))2(NC5H5)] at temperatures of (a, b) 190 °C, (c, d) 230 °C and (e, f) 270 °C. |
The powder X-ray diffraction (p-XRD) patterns of the CdS nanoparticles grown at various temperatures are shown in Fig. 5, and could all be indexed to the hexagonal phase of CdS (card number: 03-065-3414). Diffraction peaks at 2θ = 24.80°, 26.32°, 28.12°, 43.70°, 47.82° and 51.82° which correspond to the (100), (002), (101), (110), (103) and (112) planes of hexagonal CdS respectively were observed in the diffraction patterns. The high intensity and narrower (002) peak in p-XRD pattern of CdS nanoparticles indicate that the nanoparticles were elongated along the c-axis.21
CdS thin films were deposited by AACVD on glass substrates using [Cd(S2C(NC5H10))2(NC5H5)] as precursor and deposition temperatures of 350 °C, 400 °C and 450 °C. The UV-vis absorption spectra of the CdS thin films are shown in Fig. 6(a). The sharp absorption edges of the samples at ca. 516 nm confirm the energy of the optical band gap. The optical features of the CdS films were not significantly affected by deposition temperature, with an excitonic peak around 496 nm (2.5 eV); the band gaps estimated are commensurate with those previously reported for CdS thin films.39,40 The variation of the fluorescence spectrum of the CdS thin films with reaction temperature is shown in Fig. 6(b). There is one narrow and sharp emission peak in the photoluminescence (PL) spectrum due to excitonic emission for the CdS films deposited at 350 °C and 400 °C located at around 510 nm. The sharp excitonic emission peaks located near the absorption edge of the films are due to fewer surface trap states.41 CdS thin films deposited at 450 °C display a much more undefined and broader emission profile (Fig. S1, ESI†).
SEM studies show that the morphology of the CdS films change with deposition temperature. CdS films synthesized at 350 °C have regular hexagonal-like domains (Fig. 7). These structures are approximately 310 nm in size with uniform coverage on the substrate CdS films synthesized at 400 °C have a surface showing various morphological features with sizes ranging from 200 nm to 500 nm. There is a further change of morphology for films deposited at 450 °C, where close to spherical granules are observed. The coverage is non-uniform with clustered growth predominant on the substrate. Films deposited using the parent piperidine dithiocarbamate complex at similar deposition temperatures show faceted morphology with uniform film coverage (Fig. S2, ESI†). The films obtained at 400 °C show the presence of some rod-like structures. Energy dispersive X-ray spectroscopy (EDXS) at 20 kV confirmed the stoichiometry of CdS thin films deposited at 350 °C, 400 °C and 450 °C (Table 1).
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Fig. 7 SEM images of CdS thin films deposited at (a) 350 °C, magn. 20![]() ![]() |
Temperature (°C) | Cd at% | S at% | Cd/S ratio |
---|---|---|---|
350 | 50.4 | 49.6 | 1.02 |
400 | 51.5 | 48.5 | 1.06 |
450 | 53.0 | 47.0 | 1.13 |
The surface topography of the as-deposited CdS films was investigated by scanning probe atomic force microscopy (AFM). Fig. 8 shows height profiles of CdS films deposited at various temperatures on glass substrates. AFM of the CdS films deposited show the presence of uniform and crack-free surface morphologies characterized by well-interconnected spherical crystallites. The typical root-mean square roughness (Rq) was 16.9 nm, 17.8 nm and 22.7 nm at deposition temperatures of (a) 350 °C, (b) 400 °C and (c) 450 °C respectively. The increase in surface roughness with increasing deposition temperature is associated with an increase in grain size. It is evident that the deposition temperature of the thin film modifies the grain sizes as well as the surface roughness. An even and regular morphology is required for respectable performance in photovoltaic devices.42
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Fig. 8 2-D and 3-D AFM height profiles of CdS thin films deposited by AACVD at (a and b) 350 °C, (c and d) 400 °C and (e and f) 450 °C. |
The crystalline structure of the as-grown CdS thin films deposited onto glass substrates were confirmed by p-XRD using Cu Kα (λ = 1.5406 Å) radiation, with measurements in the 2θ range of 20 to 80°. The diffraction patterns of CdS thin films (Fig. 9) indicate the crystalline nature of films with the greenockite (hexagonal) structure (JCPDS card no 04-002-3090). The seven reflections at 2θ correspond to the (hkl) planes (100), (002), (101), (102), (110), (103) and (112) respectively; confirming that the product formed is pure crystalline CdS. There are no signs of any crystalline impurities such as elemental cadmium, sulfur and CdO.
Footnote |
† Electronic supplementary information (ESI) available. CCDC 984434. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c4nj01201a |
This journal is © The Royal Society of Chemistry and the Centre National de la Recherche Scientifique 2014 |