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Journal of Nanomaterials
Volume 2012 (2012), Article ID 571315, 7 pages
http://dx.doi.org/10.1155/2012/571315
Research Article

Preparation and Characterization of Self-Assembled Thin Film of MPS-Capped ZnS Quantum Dots for Optical Applications

1Department of Physics, Yildiz Technical University, Esenler, 34220 Istanbul, Turkey
2Department of Physics, Istanbul Technical University, Maslak, 34469 Istanbul, Turkey
3Faculty of Arts and Sciences, Kadir Has University, Fatih, 34083 Istanbul, Turkey

Received 25 June 2012; Revised 16 October 2012; Accepted 16 October 2012

Academic Editor: Suprakas Sinha Ray

Copyright © 2012 Kenan Koç 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.

Abstract

For this study, we prepared colloidal ZnS quantum dots using 3-mercaptopropyltrimethoxysilane (MPS) as the capping agent. Colloidal ZnS quantum dots were directly deposited on glass substrates by a spin coating process. Therefore, self-assembled films made of ZnS quantum dots in a SiO2 network were obtained using only one production step. The films were heat-treated at 100°, 125°, 150°, 175° and 200°C in an N2 atmosphere. The results showed that the dimension of quantum dots changed from 2.8 nm to 3.2 nm by heat treatment. The refractive index, extinction coefficient, thickness, and dielectric coefficient values of the films were calculated. The present study showed that size and the refractive indices of films can be controlled by the heat treatment. Therefore, such films can be a good candidate in optical filter applications.

1. Introduction

Nanoparticles have been extensively investigated due to their interesting size-dependent, optoelectronic, and physicochemical properties. Semiconductor nanoparticles belonging to II–VI group elements show significant quantum confinement effects [1]. Due to these effects, an exciting area of application of II–VI group nanoparticles is that of photonic band gap materials. Therefore, II–VI group nanoparticles can be used for the manipulation of light propagation and spontaneous emission [2]. Among these, ZnS nanoparticles have been widely used in optoelectronics such as solar cells, display panels, and optical sensors due to its wide band gap value at the visible wavelength region [3, 4]. ZnS nanoparticles and ZnS thin films can be produced by several methods [28]. One of these is the colloidal method, which has the advantages of easy production of semiconductive quantum dots, controlled size distribution, inexpensiveness, and the possibility of producing many quantum dots in a short time period.

One of the capping agents used in colloidal quantum dot production is 3-mercaptopropyltrimethoxysilane (MPS). Addition of MPS in the solvent will serve as a precursor for the growth of silica shell around the particle. Such a shell is chemically inert and optically transparent [2].

The MPS molecule has 2 functional groups. One of these is the thiol (–SH) group, which is able to make covalent bonds with different metals [9]. Therefore, –SH groups can be used to attach metallic nanostructures to the surface [10, 11]. This makes it a promising candidate for the production of quantum dots because of its ability to combine with the surface of II–VI group nanoparticles [4, 5, 1214]. The other functional group of MPS is trimethoxysilane. In most applications, MPS molecules are attached to a substrate or film surface due to the Si–O–Si bonds of the trimethoxysilane group [1417]. Trimethoxysilane is also used to make Si–O–Si bonds with MPS molecules and therefore to create SiO2 networks. Si–O–Si bonds are created with the help of hydrolysis and the condensation reactions of the sol-gel method [1417]. Producing a thin film via the sol-gel method is preferable because of its lower cost and availability in industrial production, as it is independent of the substrate geometry.

Silica is an ideal shell material for ZnS nanoparticles since its refractive index is significantly lower than the refractive index of ZnS [18]. Furthermore, SiO2 has a wide band gap (9.1 eV) and has an amorphous film structure [19]. For these reasons, some thin films are produced by introducing ZnS nanoparticles into an SiO2 matrix [1824]. Such studies usually include two production steps, and the samples are obtained using the following procedures. First, colloidal ZnS nanoparticles are produced; then the SiO2 coatings on the ZnS nanoparticle are synthesized by the sol-gel method using tetraethyl orthosilicate (TEOS) as the precursor material. Second, SiO2 sol is produced using TEOS; then the precursor solutions of ZnS are added in the SiO2 sol [2024]. On the other hand, in the present study, we prepared colloidal ZnS quantum dots using MPS as a capping agent. As explained above, MPS in the solvent was also served as a precursor for the growth of SiO2 to incorporate the quantum dots in a silica matrix [25]. Compared with other multistep procedures, in the present method, self-assembled films made of ZnS quantum dots in a SiO2 network were obtained using only one production step.

2. Experiment

2.1. Production of Quantum Dots and Thin Films

ZnS nanoparticles were produced using zinc acetate (Zn(CH3COO)2·2H2O) : thioacetamide (CH3CSNH2) = 1 molar ratio. Zinc acetate and thioacetamide were solved in methanol in two different beakers using zinc acetate : methanol = 0.02 and thioacetamide : methanol = 0.02 molar ratios. MPS (HS(CH2)3Si(OCH3)3), as the surface capping agent, was added to the beaker, including zinc acetate and methanol at MPS : Zn = 0.3 molar ratio. Finally, the two solutions in the beakers were mixed in another beaker at 60°C in an N2 atmosphere for 10 minutes. The solution with MPS-capped ZnS quantum dots was coated on Corning 2947 glass substrates using the spin coating method at 2000 rpm rotation speed for 10 seconds. The coated films were dried at 60°C for 10 minutes. Then they were heat-treated at 100, 125, 150, 175, and 200°C in an N2 atmosphere for 15 minutes. Another part of the solution was kept in laboratory conditions for 2 weeks to produce it in a gel form. Then, powdered MPS-capped ZnS quantum dots were obtained by grinding the gel. The powdered samples are used for the X-ray diffraction (XRD), high resolution transmission electron microscope (HRTEM), and Fourier transform-infrared (FT-IR) measurements.

2.2. Characterization

XRD measurements were performed using a diffractometer (GBC-MMA) operated at 35 kV and 28 mA using    radiation. HRTEM images of the MPS capped ZnS quantum dots in powder form were recorded using a JEOL 2100 HRTEM microscope operated at 200 kV. The powdered form of nanoparticles and KBr were thoroughly mixed, and the mixture was pressed to form a pellet. Then the spectrum was recorded using an FT-IR spectrometer (Perkin Elmer Spectrum One). The optical absorption spectra of the samples were recorded with a UV-visible spectrometer (Agilent 8453). Transmittance of the films was measured at a 30° angle of incidence in s and p polarizations in the spectral range of 300–1000 nm using an NKD 7000 (Aquila Instruments, England) spectrophotometer. The refractive indices, extinction coefficients, and thickness of the films were evaluated using a modified Levenburg-Marquardt procedure in a Pro-Optix data analysis software package. Transmittance curves between the 300 and 1000 nm range were fitted to the Drude-Lorentz model. The thickness of the films was determined by a profilometer (Veeco Dektak 150). The surface roughness of the film was characterized by an atomic force microscope (AFM, SPM-9500 J3, Shimadzu).

3. Results and Discussion

Figure 1 shows the XRD data for the powder of MPS-capped ZnS quantum dots. The peaks in the graph have 2  values of 28.24°, 47.72°, and 56.63° and -spacing values of 0.3157, 0.1904, and 0.1634 nm, respectively. These results correspond to (111), (220), and (311) planes and show a cubic ZnS crystal structure (JCPDS No. 77-2100).

571315.fig.001
Figure 1: XRD patterns of the MPS-capped ZnS quantum dots in powder form.

The average particle size can be found from the XRD measurements using the Scherrer equation [26] given by where    is the wavelength of the X-ray source (0.154 nm),    is the full width at half maximum of the peak at the Bragg angle, and is the coherence length. Average particle size for spherical particles, , is given by [26]. Average particle size of ZnS quantum dots was found to be 2.73 nm, using the peak corresponding to (111) plane.

The HRTEM picture of MPS-capped ZnS quantum dots is given in Figure 2. The particle size of the quantum dots was calculated from the HRTEM picture and found to be in between 2.5 and 3 nm. This value is in agreement with the particle sizes calculated from XRD measurement.

571315.fig.002
Figure 2: HRTEM picture of MPS-capped ZnS quantum dots in powder form.

The FT-IR curve of the powder form of the ZnS quantum dots is given in Figure 3. The peak at 473 cm−1 can be assigned to Si–O–Si bonding [27]. The peaks at 690 cm−1 and 917 cm−1 belong to the C–Si and Si–OH bonds, respectively [17]. The most prominent peaks of an MPS molecule in FT-IR curve at 1027 cm−1 and 1115 cm−1 belong to the asymmetric stretching of the Si–O–C and Si–O–Si bonds, respectively [17, 28, 29]. The peak at 1247 cm−1 belongs to Si–CH2–S stretching [28]. The peak at 1404 cm−1 is due to the asymmetric deformation of C–H in CH3 [30]. The peak at 1570 cm−1 may be attributed to the S–S bond [27]. The peak at 1657 cm−1 indicates the presence of C=C in the MPS molecules [31]. The peaks at 2928 cm−1 and 3143 cm−1 belong to the C–H and O–H bonds, respectively [27, 28]. FT-IR results shows that MPS molecules create an SiO2 network by producing Si–O–Si interbonds. As explained in our previous work [14], during the formation of the thin films, we suppose that quantum dots were attached to the glass surface by Si–O–Si bonds created by the OH groups of the glass surface and the Si–O groups of MPS.

571315.fig.003
Figure 3: FT-IR graph of MPS-capped ZnS quantum dots in powder form.

XRD and HRTEM measurements showed that the average radii of the nanoparticles in this study are below the excitonic Bohr radius of bulk ZnS (~2.5 nm). It is reasonable to assume a strong confinement for electrons and holes in the ZnS nanoparticles and assuming nanoparticle in a spherical box model. Absorbances of the films and their second derivative curves in the range between 250 and 350 nm are shown in Figure 4. The first exciton peak positions () were calculated from the first minimum of the second derivative of the absorbances data (Figure 4).

571315.fig.004
Figure 4: Absorbance graph of thin films forms of MPS-capped ZnS quantum dots heat-treated at different temperatures and second derivatives of absorbance spectra for the films.

Particle in a spherical box model, the first exciton peak position is given by [32] where is the band gap energy of the bulk material (3.6 eV for ZnS), is the radius of the nanoparticle, and are the effective mass values of electrons and holes, respectively, ( and for ZnS), and    is the dielectric constant (8.76 for ZnS) [33]. The average particle size of these films is calculated by inserting values into (2). Table 1 shows the values and the average nanoparticle size of these films. The sizes of the ZnS quantum dots were grown from approximately 2.8 to 3.2 nm, and the values were shifted from approximately 4.8 to 4.5 eV. These results show that the red shift of values with increasing heat treatment temperature is due to the increasing nanocrystal radius (quantum size effect). It is most likely that temperature effect causes Ostwald ripening. In that small nanocrystals are dissolved and then redeposited on to the larger nanocrystals, resulting in a larger particle size [34].

tab1
Table 1: Calculated value of particle size () by using the first exciton peak. First exciton peak () values are extracted from the second derivative of the absorbance spectra.

Figure 5 shows the optical transmittance of the films in s and p polarizations at the spectral range of 300–1000 nm. Table 2 shows the optical transmittance and their respective optical constants of the films in s and p polarizations at 550 nm for the films heat treated at 100, 150, and 200°C. Transmittance is higher for p polarization, and the results show that all of the films are transparent.

tab2
Table 2: Thickness and optical parameters (at  nm) for self-assembled thin films forms of MPS-capped ZnS quantum dots.
571315.fig.005
Figure 5: Transmittances of thin films forms of MPS-capped ZnS quantum dots in s and p polarizations.

Figure 6 shows the wavelength dependence of the refractive index, and the extinction coefficient of the films is between 300 and 1000 nm. The result showed that the refractive index decreases and the extinction coefficient increases as the heat treatment temperature rises. As expected, the refractive index values of the films were found to be between the refractive index of the bulk ZnS (2.36) [35] and that of the MPS in film form (1.45) [17]. This behaviour is similar to the results on nanocrystalline ZnS–SiO2 composite films which were previously reported by Thielsch et al. [19]. They said that “The refractive index of the composite increases with increasing concentration of ZnS from about 1.48 (the value of a pure SiO2 film) to 2.30 for a pure ZnS film.”

571315.fig.006
Figure 6: Variation of refractive index and extinction coefficient with wavelength for thin films forms of MPS-capped ZnS quantum dots heat-treated at different temperatures.

ProOptix optical data analysis software was used to calculate the thickness, and the results were checked with a profilometer (Table 2). The result showed that film thickness and refractive index decreased as the heat treatment temperature increased. Similar behaviour was previously reported by Mohamed et al. [35] for the relationship between the refractive index and thickness of nanostructure ZnS films. They showed that packing density and therefore the refractive index of ZnS films values decrease with increasing film thickness.

The complex dielectric constant is given by , where and are real, and the imaginary parts of the dielectric function can be calculated by and , respectively. Calculated real and imaginary parts of the dielectric function are given in Figure 7. The real and imaginary parts of the dielectric function of the films at 550 nm for the films heat treated at 100, 150, and 200°C are given in Table 2. The real and imaginary parts of the dielectric function show the characteristics of the refractive index and extinction coefficient, respectively.

571315.fig.007
Figure 7: Variation of real () and imaginary parts () of the dielectric function with wavelength for thin films forms of MPS-capped ZnS quantum dots heat-treated at different temperatures.

The AFM images of the ZnS thin films deposited on Corning glass substrates and heat-treated at 150°C and 200°C are shown in Figure 8. The root mean square (Rms) surface roughness of the films is 3.50 and 4.23 nm, respectively. The image shows that the root mean square surface roughness increases with the increase of annealing temperature. This will increase the pores and decrease the packing density in films which results in the decrease of refractive indices and increase of extinction coefficient of the films [36].

571315.fig.008
Figure 8: AFM images (scan area: 1.50 m × 1.50 m) of thin films forms of MPS-capped ZnS quantum dots heat-treated at 150°C and 200°C.

4. Conclusion

The present study aimed at preparation and characterization of self-assembled MPS-capped ZnS thin film of quantum dots for optical applications. Quantum dots were self-assembled directly on a glass substrate using spin coating method without introducing any matrix. Therefore, self-assembled films made of ZnS quantum dots in an SiO2 network were obtained using only one production step. This study showed that size and the refractive indices of MPS capsulated films can be controlled by heat treatment. Therefore, such type of thin films can be a good candidate in optical filter applications [37] where the main difficulty is to have a controlable refractive index and thickness.

Acknowledgments

The authors would like to thank Dr. Bahadir Keskin for the FT-IR measurement. This work is supported by the Research Fund of Istanbul Technical University.

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