group 12 dithiocarbamate complexes: synthesis, spectral studies and their use as precursors for...
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Group 12 dithiocarbamate complexes: Synthesis, spectral studies and
their use as precursors for metal sulfides nanoparticles and
nanocomposites
Peter A. Ajibade , Benjamin C. Ejelonu
Department of Chemistry, University of Fort Hare, Private Bag X1314, Alice 5700, South Africa
h i g h l i g h t s
Three dithiocarbamate complexes of
group 12 metal ions were synthesized
and characterized.
Complexes characterized by
spectroscopic techniques and
elemental analyses.
Complexes used as precursors to
prepare metal sulfide nanoparticles/
PMMA nanocomposites.
Nanoparticles sizes varied between
3.03 and 23.45 nm.
g r a p h i c a l a b s t r a c t
a r t i c l e i n f o
Article history:
Received 5 January 2013
Received in revised form 14 April 2013
Accepted 24 April 2013
Available online 7 May 2013
Keywords:
Dithiocarbamate complexes
Synthesis
Spectral studies
Precursors
Nanoparticles
Nanocomposites
a b s t r a c t
Zn(II), Cd(II) and Hg(II) dithiocarbamate complexes have been synthesized and characterized by elemen-
tal analysis, thermogravimetric analysis, UVVis, FTIR, 1H- and 13C NMR spectroscopy. The complexes
were thermolysed at 180 C and used as single molecule precursors for the synthesis of HDA capped
ZnS, CdS and HgS nanoparticles and polymethylmethacrylate (PMMA) nanocomposites. The optical and
structural properties of the nanoparticles and nanocomposites were studied by UVVis, PL, XRD and
SEM. The crystallites sizes of the nanoparticles varied between 3.03 and 23.45 nm. SEM and EDX analyses
of the nanocomposites confirmed the presence of the nanoparticles in the polymer matrix.
2013 Elsevier B.V. All rights reserved.
Introduction
Dithiocarbamate complexes are known to possess striking struc-
tural features, diversified industrial and biological applications [1].
The dithiocarbamate complexes of elements with d10 configura-
tions represent a large and interesting group of inorganic com-
pounds that have been extensively studied in recent years [25].
They have been found as useful precursors for the deposition of
II/VI compound semiconductor materials because of their reason-
able volatility and less carbon deposition as impurity [68]. Nano-
particles sizes range between 1 and 100 nm and they have wide
applications in catalysis, electronic, optical and magnetic because
of their unprecedented chemical and physical properties. They are
also used in light emitting devices, solar cells and bio-imaging [9].
The use of CdS nanoparticles in modern technology as light-emit-
ting diodes, solar cells, and optical devices based on its non-linear
optical properties has been reported. Also, ZnS semiconductor has
1386-1425/$ - see front matter 2013 Elsevier B.V. All rights reserved.http://dx.doi.org/10.1016/j.saa.2013.04.113
Corresponding author. Tel.: +27 40 602 2055; fax: +27 40 602 2094.
E-mail address: [email protected] (P.A. Ajibade).
Spectrochimica Acta Part A: Molecular and Biomolecular Spectroscopy 113 (2013) 408414
Contents lists available at SciVerse ScienceDirect
Spectrochimica Acta Part A: Molecular andBiomolecular Spectroscopy
j o u r n a l h o m e p a g e : w w w . e l s e v i e r . c o m / l o c a t e / s a a
http://dx.doi.org/10.1016/j.saa.2013.04.113mailto:[email protected]://dx.doi.org/10.1016/j.saa.2013.04.113http://www.sciencedirect.com/science/journal/13861425http://www.elsevier.com/locate/saahttp://www.elsevier.com/locate/saahttp://www.sciencedirect.com/science/journal/13861425http://dx.doi.org/10.1016/j.saa.2013.04.113mailto:[email protected]://dx.doi.org/10.1016/j.saa.2013.04.113http://crossmark.dyndns.org/dialog/?doi=10.1016/j.saa.2013.04.113&domain=pdf -
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function of temperature or time [14]. Initial decomposition for the
metal complexes starts around 130 C, 125 C, and 89 C for the Zn,
Cd, and Hg complexes respectively (Fig. 1). At a temperature of
about 223334 C about 41% of the mass of the complexes lost.
Heating the metal complexes further results into much more grad-
ual loss of mass, with about 22.85% of the mass left for the Zn com-
plex; 30.85% for the Cd complex; and 0.5% for the Hg complex- allat 800 C.
The products of the thermal decomposition of the metal com-
plexes correspond to their respective oxides, but for Hg where vol-
atilization results as observed in the thermogram. The Hg complex
initial decomposition at 30 C (0.78% mass loss) suggests the es-
cape of entrapped solvent molecule within its matrix [15]. The cal-
culated and experimental masses could be said to agree favourably
(Table 2). The mercury complex is seen to have the least stability
[16,17], the stability trend of the complexes is in the order:
Hg < Cd < Zn.
Infrared spectra studies of the metal complexes
The infrared spectra of the ligands and complexes were com-pared and assigned on careful comparison. In dithiocarbamate
complexes, three regions of great importance are: 1580
1450 cm1 due to m(CAN) of NCS; 1060940 cm1 due to m(CAS)
of CSS and 420250 cm1 due to the MAS bond [16,18]. In the free
ligands, the m(CAN) bond that appears in the range 1509
1488 cm1 shifted to 15091488 cm1 in the metal complexes.
This suggests an increase in the CAN double bond characters as a
result of the delocalization of electrons towards the metal centre
after due to coordination to the dithiocarbamate ligands [16]. In
the ligands, the m(CAS) stretching vibrations were observed as
two bands in the region 1060940 cm1. These bands occurred
as single sharp bands in the complexes at about 990 cm
1
. Thisconfirms the coordination of the ligands to the metal ions as biden-
tate chelating ligands through the sulfur atoms. The presence of
the m(CN) and m(CSS) absorption bands in the metal complexes
confirm the presence of dithiocarbamate ligands in the complexes
[19]. It has been observed in previous studies that the coordination
modes of alkyl-aryl dithiocarbamate ligands with group 12 metals
are mostly through the sulfur atoms [2022]. This is further sup-
ported by the singular absorptions which appeared at about
1000 70 cm1 region (Zn complex at1003 cm1; Cd complex at
993 cm1; and Hg complex at 992 cm1) in the FTIR spectra of
the metal complexes [16]. The characteristic frequencies of the
aromatic groups in the complexes, resulting from the out-of-plane
bending vibrations of the aromatic CAH are said to appear in the
range 600900 cm1 [23]. The (@CAH) bending modes of the aro-
matic ring was seen to absorb at around 700 cm1 in the ethyl phe-
nyl dithiocarbamate free ligand; and at about 695, 695, and
696 cm1 respectively in the Zn, Cd, and Hg complexes. The char-
acteristic absorption peak of NAH of the butyl dithiocarbamate li-
gand is seen to appear at 3281 cm1 in the free ligand and between
3208 and 3263 cm1 in the metal complexes, which is slightly be-
low the literature value of 33003500 cm1 [24].
Electronic spectra of the metal complexes
The electronic spectra of the complexes are shown in Fig. 2.
Three characteristic absorption bands are known for dithiocarba-
mate complexes due to the chromospheres NS2 caused by p?p
transition of NCS and SCS moieties; andg?p
transition arisingfrom transition of an electron of the lone pair electrons on the sul-
fur atom to an antibondingp-orbital [1]. In the metal complexes an
intense band around 291294 nm was observed due to the p?p
transition of the phenyl ring [25]. The aniline group is also said to
show a secondary band at 285 nm [26]; this band was observed be-
tween 281 and 286 in the metal complexes. The d10 electronic con-
figuration of the pseudo-transition (d10) metals is suggestive why
no dd transition over the visible region was observed [1].
NMR spectra of the metal complexes
In the 1H NMR spectra of the metal complexes two signals were
observed as multiplets around 7.447.30 ppm, which corresponds
to the aromatic protons of the phenyl ring of the ethyl phenyl moi-ety [27]. The methyl protons of the butyl group experienced up
field signals due to more shielding effect of the nuclei of the carbon
chain, and it appeared as triplets about 0.99 ppm; while the CH 3protons of the ethyl group appeared around 1.30 ppm. The peaks
Table 1
Elemental analysis of the metal complexes.
Metal complexes Formula
weight
Analytical data calculated
(found) (%)
Carbon Hydrogen Nitrogen
[(C4H9)NHCS2ZnS2CN(C2H5)C6H5] 407.98 41.18
(40.88)
4.94
(5.20)
6.86
(7.10)
[(C4H9)NH
CS2CdS2CN(C2H5)C6H5]
456.98 36. 80
(35.39)
6.13
(6.26)
4.41
(4.06)
[(C4H9)NH CS2HgS2CN
(C2H5)C6H5]
546.02 30. 77
(30.99)
3.69
(3.89)
5.13
(5.45)
Fig. 1. TGA curves showing the degradation pattern of the metal complexes.
Table 2
Thermal decomposition data of the metal complexes.
Compounds Decomposition ranges
(C)
DTG max value
(C)
Weight loss
(%)
Decomposition reaction Product
expected
Mass
changes (mg)
Cal. Found
Zn 130752 181 76.98 [(C4H9)NHCS2HgS2CN(C2H5) C6H5]? ZnS? ZnO ZnO 3.63 3.63
Cd 125340 177 68.24 [(C4H9)NHCS2CdS2CN(C2H5) C6H5]? CdS? CdO CdO 4.20 4.20
Hg 89469 144 98.89 [(C4H9)NHCS2HgS2CN(C2H5) C6H5]? HgS
volatilization
HgS 0.61 0.61
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at about 4.20 (quartets) and 3.50 ppm (triplets) are assigned to the
NACH2 protons of the ethyl and butyl groups respectively. The
methylene protons NA(CH2)2 peaks were seen at around 1.70
and 1.40 ppm in the complexes. The NH proton peak appeared
around 1.50 ppm.
In the 13C NMR spectra, two different signals were observed for
the phenyl ring attached to the N-ethyl group. The first signal ap-
peared around 145.91 ppm; while the second signal with higher
intensity was observed as three peaks between 129.14 and
126.86 ppm. This is assigned to the N-butyl group. The methylene
carbon peaks of the complexes were observed as four signals be-
tween 54.69 and 19.50 ppm. The peak observed at 78.92 ppm is
attributed to the signal of the NA(CH2) of the ethyl group which
is more deshielded than the NA(CH2) of the butyl ring. The CS2for the ZnL1L2, CdL1L2 complexes were observed at 207.87,
205.19 and 207.55, 205.44 ppm respectively.
Optical properties of the metal sulfides nanoparticles
The absorption and emission of ZnS, CdS and HgS nanoparticlesare given in Fig. 3. The peak of the spectra of the nanoparticles is
288 nm (ZnS); 291 nm (CdS) and 285 nm (HgS), which are at short-
er wavelengths than that of bulk ZnS, CdS and HgS (334, 516 and
620 nm for ZnS, CdS and HgS bulks respectively) as a result of
quantum confinement effects. This observation suggests a decrease
in the particle size of the respective nanoparticles compared to the
bulk materials. The band gap in a nanomaterial has been obtained
from the absorption maxima of their spectra. Using the fundamen-
tal absorption edges in the samples (absorption maxima), their
band gaps are calculated thus; ZnS = 4.31 eV (288 nm),
CdS = 4.26 eV (291 nm) and HgS = 4.35 eV (285 nm). The band
gap energies of the bulk samples are also calculated to be:
ZnS = 3.71 eV (334 nm), CdS = 2.40 eV (516 nm) and HgS = 2.0 eV
(620 nm) [28,29].Two emission peaks due to the exciton and the trapped lumi-
nescence are said to exist for semiconductor nanocrystals. The
exciton emission is usually observed as sharp band while the
trapped emission appears as broad band [29]. The ZnS, CdS and
HgS nanoparticles were found to exhibit emission maxima at
Fig. 2. Electronic spectra of the metal complexes.
Fig. 3. Absorption and emission spectra of the nanoparticles: (A) absorption (a) and emission (b) spectra of ZnS nanoparticle; (B) absorption (a) and emission (b) spectra ofCdS nanoparticle and (C) absorption (a) and emission (b) spectra of HgS nanoparticle.
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Fig. 4. SEM/TEM images of ZnS (A), CdS (B) and HgS (C) nanoparticles.
Fig. 5. Powder XRD pattern of ZnS nanoparticle (A); powder XRD pattern of CdS nanoparticle (B) and powder XRD pattern of HgS nanoparticle (C).
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393, 391 and 389 nm respectively. As shown in Fig. 3, a shift was
observed for all the nanoparticles with respect to absorption edge.
Fig. 4 shows the SEM/TEM pictures of samples ZnS (A); CdS (B)
and HgS (C) nanoparticles. They all gave a somewhat spherical
morphology, which agglomerated to form larger particles; thus
giving them a dense surface morphology [2931]. The nanoparticle
gave different shapes and sizes under the TEM analysis. Dots-, rice-
like- and spherical- shapes were observed for the ZnS, CdS and HgS
nanoparticles respectively. Their sizes ranged between 2.78 and
14.54 nm [29].
The XRD patterns of the metal sulfide nanoparticles are
presented in Fig. 5. The XRD patterns reveal their nanocrystalline
Table 3
Values of crystallite sizes for ZnS, CdS and HgS nanoparticles.
M et al sulfide nanop articles Angle (d eg re e) observe d maxima Full we ig ht half maxima (FWH M) Gra in siz e from XRD (nm)
ZnS 28.86 1.41 6.45
47.94 1.57 6.15
56.94 1.32 3.03
CdS 26.86 0.72 12.65
44.17 1.76 5.42
52.29 1.84 5.35
HgS 20.18 0.38 23.45
23.40 0.59 15.20
33.93 0.45 20.41
39.90 0.49 19.27
Fig. 6. SEM/TEM micrographs of the respective nanocomposites: PMMA (A); ZnS/PMMA (B/B); CdS/PMMA (C/C) and HgS/PMMA (D/D).
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natures, which indicate the broadening of the diffraction peaks due
to the higher surface to volume ratio [28]. ZnS nanoparticle
showed broad peaks at 2h = 28.86, 47.95 and 56.94, which can
be indexed to (111), (220) and (311) planes of cubic zinc blende
structure (JCPDS 05-0566) Fig. 3 [28,29]. The three peaks ob-
served in the XRD patterns of CdS nanoparticle correspond to
(111), (220) and (311) of the cubic crystal phase of CdS (JCPDS
5-0566) [32]. The XRD patterns (111), (200), (220) and (311) ob-tained for HgS nanoparticle are in agreement with the pattern
JCPDS 00-006-0261, which correspond to HgS metacinnabar, syn
[29]. The ZnS and CdS samples appeared to be of much more smal-
ler particle sizes than that of HgS as indicated by the observed rel-
atively broader diffraction peaks for the ZnS and CdS nanoparticle
XRD patterns compared to that of HgS nanoparticle (Fig. 5AC). Ta-
ble 3 contains the values of crystallite sizes for ZnS, CdS and HgS
nanoparticles.
Structural properties of the metal sulfide/PMMA nanocomposites
SEM was used to study the morphology and the extent of inter-
action of the ZnS, CdS and HgS nanoparticles with PMMA. Fig. 6A
shows the SEM image of PMMA, while Fig. 6BD shows the SEM
images of ZnS/PMMA, CdS/PMMA and HgS/PMMA respectively.
The SEM monograph obtained for the polymer (PMMA) shows a
well-defined shape of spherical aggregates [33,34]. The pro-
nounced spherical aggregates observed in PMMA micrograph were
somehow lost (dissolved) in the PMMA interaction with different
nanoparticles; thus suggesting an interfacial interaction between
the polymer and the metal sulfide nanoparticles. The TEM images
revealed that some interaction occurred between the inorganic
nanoparticle materials and the polymer, which has been observed,
could help to increase the stability of the pure PMMA polymer and
hence, enhance its usability [33]. The chemical composition of the
metal sulfide/polymer nanocomposites were studied by EDX,
which confirmed the presence of Zn, S; Cd, S and Hg, S from ZnS,
CdS and HgS nanoparticles respectively.
Some broadening of the diffraction peaks and the decrease ofthe intensity of the spectra were observed in the XRD patterns of
the nanocomposites. This may be attributed to the pore filling ef-
fects, which is said to reduce the scattering contrast between the
pores and the frame work PMMA materials [3537].
Infrared spectral studies of the nanocomposites
The FTIR data revealed that the absorption band patterns of the
ZnS/PMMA, CdS/PMMA and HgS/PMMA nanocomposites are simi-
lar to those of the pure PMMA. However, a slight shift was ob-
served in their stretching frequencies suggesting the possibility
of an interaction between the metal sulfide nanoparticles and the
polymer. This possible interaction between the inorganic and or-
ganic phases could influence the thermal stability of the purePMMA [32,33].
Conclusion
Zn(II), Cd(II) and Hg(II) complexes of some alkyl-phenyl dithio-
carbamates were synthesized and characterized by elemental anal-
ysis, TGA, UVVis, FTIR, 1H- and 13C NMR spectroscopy.
Spectroscopic analyses confirmed the coordination of the metal
ions to the dithiocarbamate anions acting as bidentate chelating li-
gands. The complexes were used as single molecular precursors to
synthesize ZnS, CdS and HgS nanoparticles and PMMA nanocom-
posites. The crystallites sizes of the nanocomposites varied be-
tween 3.03 nm and 23.45 nm. EDX analysis from the SEM of the
nanocomposites confirmed the presence of the nanoparticles in
the polymer matrix and the broadening observed in the XRD of
the nanocomposites of the nanocomposites also confirmed the for-
mation of the nanocomposites.
Acknowledgements
The author acknowledged with thanks financial support from
Govan Mbeki Research and Development Centre, University of Fort
Hare. BCE acknowledged Adekunle Ajasin University, Akungba
Akoko, Nigeria for study leave to undertake this study.
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