Synthesis, Morphology, and Optical Properties of Au/CdS Hybrid Nanocomposites Stabilized by Branched Polymer Matrices

Chumachenko, V. A.; Naumenko, A. P.; Yeshchenko, O. A.; Kutsevol, N. V.; Bondarchuk, I. S.

doi:https://doi.org/10.1155/2016/1439437

Journal of Nanomaterials

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Abstract Introduction Results and Discussion Conclusions Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2016 | Article ID 1439437 | https://doi.org/10.1155/2016/1439437

Synthesis, Morphology, and Optical Properties of Au/CdS Hybrid Nanocomposites Stabilized by Branched Polymer Matrices

V. A. Chumachenko,¹A. P. Naumenko,²O. A. Yeshchenko,²N. V. Kutsevol,¹and I. S. Bondarchuk²

Academic Editor: William Yu

Received28 Jan 2016

Revised22 Mar 2016

Accepted04 Apr 2016

Published21 Apr 2016

Abstract

Metal/semiconductor (Au/CdS) nanocomposites were synthesized in the solution of branched D-g-PAA polymer. TEM and DLS of Au/CdS/D-g-PAA nanocomposites revealed complicated nanocomposite structure consisting of the Au nanoparticles (NPs) of 6 nm in size surrounded by small CdS NPs with size of 3 nm. These nanocomposites formed the aggregates-clusters with average size of 50–800 nm. Absorption spectra of Au/CdS nanocomposites consist of the bands of excitons in CdS NPs and surface plasmons in Au ones. The surface plasmon band of gold NPs is red shifted and broadened in Au/CdS/D-g-PAA nanocomposites comparing to the one of Au NPs in Au/D-g-PAA proving the fact of close location of CdS and Au NPs in the synthesized Au/CdS/D-g-PAA nanocomposites. The PL spectra of Au/CdS nanocomposites originate from the radiative transitions in excitons in CdS NPs. The 4-fold increase of intensity of free exciton PL is observed for CdS NPs in Au/CdS/D-g-PAA comparing to CdS ones in CdS/D-g-PAA that is due to PL enhancement by local field of surface plasmons of Au NPs. Also, the 12-fold decrease of intensity of localized exciton PL is observed for CdS NPs in Au/CdS/D-g-PAA comparing to CdS ones in CdS/D-g-PAA. Most probably, it is due to passivation of the surface of CdS NPs carried out by the Au ones.

1. Introduction

Semiconductor nanoparticles are of great interest for both fundamental research and industrial development because of their exciting utilization in the areas of light-emitting diodes, electroluminescent devices, lasers, hydrogen producing catalyst, biological labeling, and immune diagnosis [1–7]. On the other hand, in recent decades, there has been a huge interest in metal-based plasmonic nanostructures for applications in biosensing, nanophotonics, and enhanced light emission [8–10]. This is due to the collective coherent excitations of the free electrons in nanosized metal, also known as surface plasmon resonance (SPR). Surface plasmons (SPs) give rise to the enhancement of the local electric field close to the surface of metal NPs. Such strong local electric field enhances the optical processes such as surface enhanced Raman scattering (SERS) [11–13] and surface enhanced photoluminescence (SEPL) [14–18] in molecules, clusters, and NPs of dielectrics and semiconductors located near the surface of metal NPs or close to a rough metal surface. If the molecule is close to the metal NP, the metal NP couples to the molecule through the plasmonic field. So, the metal NP acts as a nanoantenna in the sense that it channels the excitation light to the molecule and directs its photoluminescence (PL) to the far field more efficiently as compared to the free molecule.

Recently, the growing ability to fabricate metal/semiconductor (M/S) composites, Au/CdS ones in particular, on a nanoscale has opened new opportunities for designing multifunctional materials [19–25]. The use of these new materials then requires identifying and understanding the emergence of new properties due to the combination of different material systems on the nanometer length scale. The optical properties of these nanostructures, for example, often exhibit interesting deviations from their individual components. These optical effects include a shift in the surface plasmon resonance of noble metal NPs when combined or coated with other materials [26, 27] or changes in the PL intensity of semiconductor NPs which can be attributed to the overlap of the electronic structures of the different components [28]. Multicomponent hybrids show advantages over single component materials due to the external light activity benefiting from the synergistic effect among different components. A popular approach to increasing the visible light activity is to integrate the metal NPs with strong plasmonic feature into the multicomponent nanostructures. One attraction of such approach is that the plasmonic metal NPs could serve as sensitizers, enabling the visible light utilization by wide bandgap semiconductors. The plausible design/fabrication strategies are still somewhat unclear and under intensive debating and investigating.

Current paper presents the characterization of Au, CdS NPs, and Au/CdS hybrid nanocomposites synthesized into branched D-g-PAA polymer matrices. The size and shape of NPs are actually controlled by the choice of the synthesis route, the protection agent, and the synthesis conditions [26]. Due to high reactivity of NPs the preparation of stable nanosystems requires a protection agent preventing a possible aggregation process [29]. Polymers are commonly used as stabilizing agents. They enhance the stability of NPs by introducing steric and/or electrostatic repulsion between them. On the other hand, polymers can also play a role in the process of the in situ NP formation, namely, in the control of their size and morphology. In our previous research it was shown that branched polymers are more efficient in this aim in comparison with linear analogues [30–33]. The comparative analysis of the optical properties of Au/D-g-PAA, CdS/D-g-PAA, and Au/CdS/D-g-PAA was performed. The mutual influence of Au and CdS NPs on their absorption and PL spectra was observed. In particular, we observed the sufficient enhancement of the free exciton photoluminescence in CdS NPs by the plasmonic field of Au NPs. Also, the quenching of the luminescence of localized excitons in CdS NPs occurring due to possible passivation of the surface of CdS ones was observed.

2. Experimental Details

2.1. Materials

CdSO₄, Na₂S, HAuCl₄, and NaBH₄ were purchased from Aldrich and used without additional purification. Branched star-like copolymer dextran-g-polyacrylamide (D-g-PAA) was used as a matrix for in situ CdS and Au/CdS synthesis. The polymer plays role of matrix to act as nucleating, capping, and stabilizing agent simultaneously.

The copolymer was obtained by free radical polymerization initiated by ceric ion reducing agent. Namely, copolymer polyacrylamide chains were grafted onto dextran core ( = 7 × 10⁴ g/mol) [34, 35]. The redox process initiates free radical sites exclusively on the polysaccharide backbone, thus preventing from the formation of PAA homopolymers.

Synthesis, identification, and analysis of the polymer average structure were described in [34, 35]. The theoretical numbers of grafting sites per dextran backbone for the samples we use in the present work are equal to 5, so the related D-g-PAA copolymers are referred to as D70-g-PAA5. The molecular characteristics of branched polymer obtained by size exclusion chromatography were the following: = 1.57 × 10⁶ g/mol; = 1.81; and = 85 nm.

This copolymer has star-like structure, consisting of a compact dextran core and long polyacrylamide arms [34]. The structure peculiarities of branched polymers, causing higher local concentration of functional groups in comparison with their linear analogue, give the advantages for application of branched polymer systems in nanotechnologies [36].

2.2. Polymer Characterization

Size exclusion chromatography (SEC) was carried out by using a multidetection device consisting of a LC-10AD Shimadzu pump (throughput 0.5 mL/min), an automatic injector WISP 717+ from Waters, 3 coupled 30 cm Shodex OH-pak columns (803HQ, 804HQ, and 806HQ), a multiangle light scattering detector DAWN F from Wyatt Technology, and a differential refractometer R410 from Waters. Distilled water containing 0.1 M NaNO₃ was used as eluent.

2.3. Synthesis of Au/D-g-PAA and CdS/D-g-PAA Nanocomposites

Au NPs were synthesized by the chemical reduction of Au precursor (HAuCl₄) dissolved in polymer aqueous solution (pH = 5.5). 0.24 mL of 0.1 M HAuCl₄ aqueous solution was added to 10 mL of aqueous polymer solution ( = 2 × 10⁻³g/cm³) and stirred for 20 min. Then, 0.94 mL of aqueous solution of NaBH₄ (0.1 M, 3.8 × 10⁻³g/cm³) was added. The final aqueous solution was stirred for 30 min. It turned ruby-red in colour; thus the formation of Au NPs was indicated.

CdS NPs synthesis was carried out in the solution of polymer at room temperature (25°C). Stock solution of CdSO₄ (0.1 М, 2.084 × 10⁻³g/cm³) and Na₂S (0.1 M, 7.8 × 10⁻³g/cm³) in deionized water was prepared. 0.9 mL of CdSO₄ solution was added to 20 mL of aqueous polymer solution ( = 10⁻³g/cm³), the mixture was stirred for 15 minutes, and then 0.9 mL of the Na₂S stock solution was injected under stirring. The resulting stable yellow CdS colloids were characterized in 24 h and then remained essentially unchanged for at least 4 months.

2.4. Synthesis of Au/CdS/D-g-PAA Hybrid Nanocomposites

In the first stage the Au NPs were synthesized by the chemical reduction of Au precursor (HAuCl₄) dissolved in polymer aqueous solution at = 25°C in aqueous solutions of dextran-graft-polyacrylamide copolymer (D70-g-PAA5). 0.24 mL of 0.1 M HAuCl₄ aqueous solution was added to 10 mL of aqueous polymer solution ( = 2 × 10⁻³g/cm³) and stirred for 20 min. Then, 0.94 mL of aqueous solution of NaBH₄ (0.1 M, 3.8 × 10⁻³g/cm³) was added. The final aqueous solution was stirred for 30 min. It turned ruby-red in colour; thus the formation of Au NPs was indicated. Then 0.9 mL of CdCl₂ solution was added to 5 mL Au precursor solution, the mixture was stirred for 15 minutes, and then 0.9 mL of the Na₂S stock solution was injected under vigorous stirring. The resulting stable dark-brown colloids were characterized in 24 h and then remained stable in 4 months.

2.5. Characterization

2.5.1. Transmission Electron Microscopy

For the sample preparation 400-mesh Cu grids with plain carbon film were rendered hydrophilic by a glow discharge treatment (Elmo, Cordouan Technologies, Bordeaux, France). A 5 μL drop was deposited and left to adsorb for 1 min; then the excess of solution was removed with a piece of filter paper. The observations of the Au NPs were carried on two TEMs, Tecnai G2 or CM12 (FEI, Eindhoven, Netherlands) and the images were acquired with ssCCD Eagle camera on the Tecnai and a MegaView SIS Camera on the CM12. Image analysis was carried out using the open-source software ImageJ. The NPs’ diameters () were estimated from NPs’ areas () as . Over a dozen of TEM images and at least 300 particles for each sample were processed for size distribution analysis in order to obtain reliable data. Gauss fitting was carried out to estimate mean radius and standard deviation of the distribution.

2.5.2. Dynamical Light Scattering (DLS)

DLS measurements were carried out using Zetasizer Nano ZS90 (Malvern Instruments Ltd., UK). The apparatus contains a 4 mW He-Ne laser with a wavelength 632.8 nm and the scattered light is detected at an angle 60°. To estimate hydrodynamic radius distributions from correlation functions, CONTIN algorithm [37], known to be applicable for complicate multicomponent systems [38], was applied using MATLAB code. At least 10 correlation functions were processed for each sample.

2.5.3. Optical Spectroscopy

A tungsten-halogen incandescent lamp was used as the light source for absorption measurements. The single-grating spectrometer MDR-3 was used for the registration of absorption spectra. PL spectra of the samples were measured using Cary Eclipse (Varian Inc.) fluorescence spectrophotometer. The PL was excited by a single monochromatic line with wavelength of 300 nm (spectral half-width of 5 nm) cut from the continuous emission spectrum of a pulse Xe lamp. The repetition rate of the pulses was 80 Hz, pulse duration was 2 μs, and pulse power density was 1.3 × 10³ W/cm². Original solutions were diluted 25 times before spectral measurements.

3. Results and Discussion

3.1. Morphology

TEM images of Au and СdS sols as well as Au/CdS nanocomposite are represented in Figures 1–3. The individual sols of Au and CdS were prepared and studied to understand the Au/CdS nanocomposites structure. The TEM images of Au sol (Figure 1(a)) reveal the existence of the single particles of nm in size and their aggregates with size up to 60 nm, respectively. The TEM images of CdS sols confirm the presence of the single CdS particles of in size as well as the aggregates of percolated particles (Figures 2(b) and 2(c)). Individual CdS NPs are well defined and are nearly spherical (Figure 1(b)). It is evident that single CdS NPs are not dispersed regularly in the sol but form local structures-clusters with average size of 50–200 nm (Figure 2(c)). TEM image analysis of Au/СdS sols revealed complicated nanocomposite structure (Figure 3(a)). We can observe the Au NPs of nm in size surrounded by small CdS particles with size of nm (Figures 3(b) and 3(c)). These nanocomposites form the aggregates-clusters (Figure 1(a)) with average size of 50–800 nm. The Au NPs are well defined (dark grey) in the Au/CdS nanocomposite and have spherical shape. The CdS NPs are grey and dispersed around Au NPs.

(a)

(b)

DLS results evaluated for these nanosystems are shown in Figure 4. DLS results analysis for all nanosystems synthesized in branched polymer matrix (Figure 4(a)) is in good agreement with TEM (Figures 1–3). Synthesized sol included 2 fractions of Au NPs, namely, nm and nm. For CdS sols the existence of aggregates having average size of 20–80 nm (Figure 4(b)) is observed. That confirmed the TEM results. Taking into account TEM images, DLS results analysis, molecular parameter of polymer ( = 85 nm), and synthesis condition, it can be suggested that the single CdS NPs have been grown directly in the polymer molecule and form the clusters localized in limited macromolecule volume. DLS results for Au/CdS nanocomposites reveal the existence in the sols of the aggregates-cluster from 20 to 1000 nm in size (Figure 4(c)). It can be also concluded that Au/CdS nanocomposites are fabricated into the polymer molecule and form the clusters localized in limited macromolecule volume.

(a)

(b)

(c)

3.2. Optical Properties

The light absorption and photoluminescence (PL) spectroscopy was used for optical characterization of fabricated nanocomposites. Room temperature optical absorption spectrum of the CdS NPs in D-g-PAA (Figure 5, blue dotted line) exhibits two bands labeled as and with maxima at 415 nm and 457 nm, respectively. These bands are due to the transition in CdS NPs between the ground and first excited exciton states in single NPs and aggregated ones correspondingly [39–41]. Also, it is seen from Figure 5 that the absorption spectrum of Au NPs in D-g-PAA (Figure 5, green dashed line) demonstrates the clear surface plasmon resonance (SPR) band [42–44] with maximum at 536 nm. The absorption spectrum of Au/CdS/D-g-PAA hybrids dispersed in water is shown in Figure 5 (red solid line). This spectrum exhibits three absorption bands with maxima at 548 nm, 417 nm, and 460 nm which are SPR, , and ones corresponding to SPR excitation in Au NPs as well as to excitonic transitions in single and aggregated CdS NPs.

Let us note that the surface plasmon band of Au NPs in Au/CdS/D-g-PAA hybrid nanostructures is red shifted (548 nm) comparing to Au NPs in Au/D-g-PAA (536 nm); that is due to the sensitivity of SPR to changes in the dielectric permittivity of the surrounding medium . Indeed, the dielectric permittivity of CdS is higher than the one of polymer. Since the SPR frequency depends on as , where is the bulk plasmon frequency, the increase in leads to decrease of , that is, to the red shift of SPR. Thus, the absorption spectrum indicates that in Au/CdS/D-g-PAA hybrid nanostructures the Au NPs are surrounded by CdS ones. This conclusion is in agreement with TEM images (Figure 3(a)) showing that small CdS NPs are grouped around larger Au ones. Also, it is seen from Figure 5 that the plasmonic absorption band decreases in intensity and broadens in comparison with sole Au NPs in Au/D-g-PAA system. This indicates the fact of increase of plasmon damping. It is known that increase of the plasmon-exciton coupling strength can result in the enhancement of the absorption in CdS NPs and the suppression of the plasmon absorption in Au NPs [45]. This enhancement would benefit in the construction of the active layer of photovoltaic solar cell to increase their efficiency. The second cause of SPR band broadening can be the fluctuations of dielectric permittivity of the surrounding medium [46, 47]. Such fluctuations are originated from the random location of CdS NPs in the vicinity of Au ones. These fluctuations cause fluctuations of SPR frequencies in different gold NPs, which leads to the spectral broadening of SPR absorption band.

Room temperature PL studies were performed as well. The PL spectrum of the CdS NPs in D-g-PAA (Figure 6, blue dotted line) exhibits three bands labeled as , , and XD with maxima at 415 nm, 477 nm, and 650 nm, respectively. and bands correspond to the respective absorption and ones and are due to the radiative transitions in CdS NPs between the first excited and ground exciton states in single CdS NPs and aggregated ones. Also, an additional XD band is due to radiative transitions in CdS NP excitons localized on the defects [48]. Taking into account that defect XD band dominates in the spectrum, one can conclude that the synthesized CdS NPs have quite defected structure. Since CdS NPs are quite small, it is reasonable to assume that these defects are surface ones. The PL spectrum of Au/CdS/D-g-PAA hybrids dispersed in water is shown in Figure 6 by red solid line. This spectrum is quite surprising; namely, the intensity of localized excitons’ XD band decreased hugely (6.5 times), while the total intensity of free excitons’ and bands increased significantly (3.2 times). It is interesting that a similar result was obtained when the solution of Au NPs in D-g-PAA was mixed with the solution of CdS NPs in D-g-PAA (Au+CdS/D-g-PAA mixture). The PL spectrum of such mixture is shown in Figure 6 by green dash-dotted line. One can see that the intensity of XD band decreases (12 times) and the total intensity of and ones increases (4 times) even more than for Au/CdS/D-g-PAA hybrids. One can suppose that so strong decrease of defect XD band is due to some passivation of the surface of small CdS NPs carried out by Au ones. Indeed, as we noted above in Au/CdS/D-g-PAA system, the small CdS NPs are located around the larger Au ones. In Au/CdS/D-g-PAA composite the CdS NPs are located in the vicinity of Au ones (the distances between Au NPs and CdS ones are several tens of nm, which is seen in TEM image, Figure 3). Thus, CdS NPs are located in the dipolar plasmonic field of Au NPs which enhances the exciton radiative transitions in CdS ones. Such enhancement leads to significant increase of intensity of PL of free excitons in CdS NPs.

The increase of intensity of the free exciton and bands for Au+CdS/D-g-PAA mixture and the decrease of defect XD band show that CdS NPs are located in the vicinity of Au ones. Note that it looks quite surprisingly since both CdS and Au NPs are surrounded by polymers which would cause the steric repulsion for NPs. To check the fact that CdS and Au NPs are located close to each other we measured the absorption spectrum of the CdS+Au/D-g-PAA mixture (green dash-dotted line in Figure 5). One can see that SPR band is red shifted and broadened in CdS+Au/D-g-PAA system comparing to SPR one in Au/D-g-PAA system (orange dashed line) which is similar to the behaviour of SPR band in hybrid CdS/Au/D-g-PAA system (red solid line). As it is noted above, such shift and broadening reflect the influence of CdS NPs on the SPR in Au ones proving the fact that CdS NPs are located in the vicinity of Au ones. Thus, one can conclude that in Au+CdS/D-g-PAA mixture the diffusion of CdS and Au NPs occurs leading to close location of these NPs in resulting mixture nanocomposite.

4. Conclusions

In conclusion, the metal/semiconductor (Au/CdS/D-g-PAA) nanocomposites were synthesized in the solution of branched D-g-PAA polymer. Polymer controlled the size and morphology of NPs in the process of their synthesis and was a stabilizing agent for sols. The nanosystems containing only Au NPs or only CdS ones were obtained for comparative studies. TEM and DLS of Au/CdS/D-g-PAA nanocomposites results were in good agreement and revealed complicated nanocomposite structure consisting of isolated and aggregated Au NPs surrounded by small CdS NPs. These nanocomposites formed the aggregates-clusters with average size of 50–800 nm. It can be also concluded that Au/CdS/D-g-PAA nanocomposites form the clusters localized in limited macromolecule volume. Optical absorption spectrum of Au/CdS/D-g-PAA nanocomposites exhibits three absorption bands at 415 nm, 460 nm, and 548 nm that originate from the excitation of excitons in single and aggregated CdS NPs and surface plasmons in Au ones, respectively. The surface plasmon band of gold NPs red shifts and broadens in Au/CdS/D-g-PAA nanocomposites comparing to the case of sole Au NPs in Au/D-g-PAA. This is due to the fact that in Au/CdS/D-g-PAA system the gold NPs are surrounded by small CdS ones, which leads to increase of the local dielectric permittivity of environment of Au NPs. The PL spectra of Au/CdS/D-g-PAA nanocomposites consist of three bands at 415 nm, 477 nm, and 650 nm, respectively, that correspond to radiative transitions in free excitons excited in single and aggregated CdS NPs and the excitons localized on lattice defects in CdS ones. A quite unexpected result was obtained, which is that in the presence of Au NPs the intensity of PL band of localized excitons in CdS NPs decreases hugely (6.5 times) while the intensity of PL bands of the free excitons sufficiently increases (3.2 times). Most probably, the strong decrease of localized exciton band is due to passivation of the surface of small CdS NPs carried out by the Au ones. Meanwhile, the significant increase of intensity of PL of free excitons is due to the enhancement of radiative excitonic transitions in CdS NPs by field of surface plasmon in Au ones.

Competing Interests

The authors declare that they have no competing interests.

Acknowledgments

O. A. Yeshchenko and I. S. Bondarchuk acknowledge the support by the NATO Science for Peace and Security (SPS) Program (Grant NUKR.SFPP 984617).

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Copyright © 2016 V. A. Chumachenko et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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