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Synthesis and studies on structural and optical properties of zinc oxide and manganese-doped zinc oxide nanoparticles
S. Ajin Sundar1, N. Joseph John2 department of Physics, Government Arts College, Udhagamandalam, Tamilnadu, India. Pin - 643002 2 Department of Physics, Sethupathy Government Arts College, Ramanathapuram, Tamilnadu, India.
Pin - 623502
njosephjohn@gmail.com
DOI 10.17586/2220-8054-2016-7-6-1024-1030
Wet chemical techniques have been used to synthesize undoped and Mn-doped nanoparticles at room temperature. Highly stable pure and 5.0 weight% Mn-doped ZnO nanoparticles have been prepared. The morphologies, structures and optical properties of the as-prepared samples were characterized by X-ray powder diffraction, scanning electron microscopy, energy dispersive X-ray spectroscopy and UV-Vis spectra. The results clearly reveled that both the pure and doped samples had a wurtzite hexagonal phase. The SEM studies illustrated that grain size decreases with Mn doping, with average diameter ~30 nm, which is in good agreement with the average crystalline size calculated by Scherrer's formula. The strong absorption band in the UV region for the prepared samples can be attributed to the band edge absorption of the wurtzite hexagonal ZnO.
Keywords: nanoparticles, X-ray techniques, structural, FTIR, SEM, EDX. Received: 1 March 2016 Revised: 25 August 2016
1. Introduction
Due to its wide band gap (^3.37 eV) and large exciton binding energy (^60 meV), ZnO is of great interest for photonic applications and its optical properties have been studied in detail. In recent years, due to prediction of possible ferromagnetic properties in transition metal-doped ZnO with Curie temperatures (Tc) above room temperature, studies of transition metal doped ZnO have attracted much interest [1,2]. Multifunctional materials come on stage accompanied with magnetic properties in diluted magnetic semiconductors (DMS), in which nonmagnetic ions replace some of the magnetic and non-magnetic cations. The origin of ferromagnetic properties in diluted semiconductors have been theoretically and experimentally studied [3,4].
Among DMS materials, ZnO-based DMS has remarkable features: (i) Direct wide band gap at room temperature, (ii) access to the large bulk and high-quality single crystals of ZnO and (iii) large exciton binding energy. The latter is useful for having lasers with high efficiencies at room temperature [5,6]. In addition, ZnO is useful in solar cells and sensors as it is transparent conductive and piezoelectric [7]. Pure ZnO nanostructures show weak optical features that result from point defects such as oxygen vacancy or interstitial Zn; therefore, they cannot be used directly in the industry [7]. As a result, doping ZnO with a convenient element is a method for engineering optical and magnetic properties. Furthermore, in order to make optoelectronic devices, n-type and p-type states are needed. It is relatively difficult to achieve p-type doping and this limitation is considered an obstacle to using ZnO in these applications [8].
Additionally, ZnO is lower in cost and is environmental friendly as compared to other metal oxides [9]. Normally, ZnO is studied in nanoscale; this is probably due to the fact that the high surface area to mass ratio of nanoparticles could enhance the adsorption of organic pollutants on the surface of particles as compared to the bulk materials [10]. Thus, in order to enhance the optical, magnetic, and electrical properties of ZnO, transition metal-doped ZnO nanoparticles have been introduced. The modification of ZnO nanoparticles by impurity incorporation leads to possible application in UV optoelectronic and spin electronics [11]. Among the transition elements, Mn shows the maximum magnetic behaviors with electron effective mass ~0.3me (me= free electron mass); a doping of Mn into the ZnO semiconductor host lattice may result in large injected spins and carrier which make it suitable to be applied as diluted magnetic semiconductor (DMSs) [12].
ZnO has penetrated far into industry, and is one of the critical building blocks in modern society. Zinc oxide is in all likelihood one of the most abundant forms of any known material. The properties of ZnO are strongly dependent on its structure, including the morphology, aspect ratio, size, orientation, and crystal density. Due to its potential application in many areas, such as optoelectronic devices, solar cells, chemical sensor, and photocatalyst hence, ZnO has attracted much attention from researchers and scientists to develop it for technological applications.
The term "doped" is used to modify the optical or magnetic properties of the host by adding impurities ions which become incorporated into the host lattice. Doping with 3d metals such as Mn, Ni, Fe, Co, and Cr will increase the surface area and reduce the particle size of ZnO nanoparticles [13]. Mn is preferred for the doping of ZnO because the d electron of Mn at t2g level can easily overlap with the ZnO's valence bond, as compared with other transition elements. Among nanomaterials of transition metal oxides, ZnO is considered as a significant material for multiple applications, including catalytic, optical, magnetic, electrical, electrochemical and biological uses. These properties makes ZnO as a multifunctional material that finds applications in solar cell, biosensors, field effect transistors, light emitting diodes, diluted and ferromagnetic materials for spintronics, photocatalysis and anti-bacterial activity [13]. There are various studies which have shown that Mn-doped semiconductors have influenced the physical, chemical, and structural properties of undoped ZnO nanoparticles. For example, the optical properties of undoped ZnO nanoparticles especially on the tuning of the band gap can be greatly improved at the nanoscale by optimum Mn doping content [14,15].
It was observed that doping with 3d metals reduced the Eg of semiconductors by forming interband-gap localized levels [16]. The charge-transfer transition between the d-electron of dopant (t2g levels) and the conduction band (CB) or valence band (VB) was reported [17]. Conversely, the metal's d-orbitals are mixed with the CB and VB of the semiconductors [18]. This overlap is because wide VB or CB directly decreases Eg. Recently, there has been much attention focused on modifying ZnO by doping with transition metals, such as Ag [19], Ni [20], Cu [21], Co [22], Cr [23], Ti [24]. These studies demonstrated that the metals can change the Eg of ZnO, and that the dopants can alter the ZnO grain size. This also demonstrated the presence of the d-electron because the t2g of manganese (Mn) is very close to the VB [17,25]. More recently, the synthesis of a Mn-doped ZnO nano-crystal (not powder) was reported by wet-chemical techniques [26]. Moreover, ZnO nanocrystalline powders doped with
1, 3 and 5% Mn were prepared using a sol-gel process [27].
Zinc oxide is a II-VI compound semiconductor. Its properties, such as wide bandgap, large excitation binding energy and low threshold power for optical pumping are considered to be the eminent features of ZnO. Thus, ZnO is said to be an efficient phosphor [28-31]. Type II-VI semiconductors, as a class of materials, have been and still are the subject of much intensive investigation. The growth of semiconductor technology in the early 1950's highlighted the limitations of silicon and germanium, which perhaps the character and the magnitude of the forbidden energy gap were the most disadvantageous. At first the extension in the range of energy gaps was sought in these III-V semiconductors, where considerable success has been achieved with InSb and GaAs in the low and high energy gap areas respectively. GaAs is today probably the most developed and well understood compound in existence. Concurrently with the later developments in the III-V semiconductors, systematic studies were made for several of these compounds.
The results of these studies have revealed much about the general nature of the II-VI semiconductors and the feature of chemical stability of the higher energy gap materials at room temperature offers an immediate advantage over the unstable III-V phosphides. Type II-VI semiconductors, in their broadest sense, include compounds formed from elements of group II and group VI of the periodic table. Zinc oxide has a wide band gap large excitation energy of 60 meV, high chemical stability, good piezo-electric properties, nontoxicity and biocompatibility. To synthesize ZnO nanoparticles with transition metals, several different methods have been employed, such as wet chemical methods like sol-gel [32], co-precipitation [33], combustion [34] etc. These nanoparticles have been used in a wide range of applications, such as sensors, varistors, piezoelectric, transducers, surface acoustic wave devices, phosphors, transparent conducting oxides, optoelectronic devices, ferromagnetic devices, and heterogeneous photo catalysts [35-40]. In this paper we report the synthesis and characterization of Mn doped and undoped zinc oxide via wet chemical method as well as the effect of 5.0 wt% Mn doping in ZnO on its structural, morphological and optical properties.
2. Experimental
2.1. Materials Used
Analytical Reagent (AR) grade Zinc acetate dehydrate, Sodium Dodecyl sulfate, Sodium hydroxide and manganese chloride were used for synthesis of pure and manganese doped zinc oxide nanoparticles. Reagents were purchased from Merck India and used as received without any further purification.
2.2. Synthesis of ZnO Nanoparticles
For the synthesis of pure zinc oxide nanoparticles 10.966 g of zinc acetate dihydrate was added to 250 ml water with vigorous stirring until an homogeneous solution was obtained. Next, 10.974 g of NaOH was added to the solution under stirring and to this solution 14.4 g of sodium dodecyl sulfate was added under continuous
stirring until a pH of 12 was reached. This solution was was dried in a hot air oven at 160 °C overnight. The material was then ground in a mortar and pestle and the powder thus obtained was washed several times using ethanol and deionized water. The product was then dried at 60 °C overnight and the obtained product was calcined at 500 °C for 4 hours.
2.3. Synthesis of Mn-Doped ZnO Nanoparticles
For the synthesis of 5.0 weight% manganese doped ZnO, 0.7916 g manganese chloride was added to 250 ml of water under vigorous stirring and 10.966 g zinc acetate was then added. Next, 10.974 g of sodium hydroxide was added to the solution with 14.4 g sodium dodecyl sulfate added under continuous stirring till the pH value reached 12 and the solution was dried in a hot air oven at 160 °C overnight. Then the material was taken and ground using a mortar and pestle and the obtained powder was washed several times using ethanol and deionized water. The product was dried at 60 °C for 2 days and the obtained product was then calcined at 500 °C for 4 hours.
2.4. Characterization Studies
The pure and manganese doped Zinc oxide nanoparticles thus obtained were characterized by UV, FTIR, XRD, SEM and EDAX. The seven synthesized samples were characterized using UV-visible spectroscopy by dissolving 0.1 g of each sample in 100 ml doubly distilled water. The absorption data was recorded as a function of wavelength using a UV-visible spectrophotometer model-2202, India. XRD (X-ray Powder Diffraction) is rapid analytical technique primarily used for phase identification of crystalline material. The average crystallite size was determined from XRD peaks using Scherer's formula. The field emission Scanning Electron Microscopy (SEM) is one of the most versatile and well known analytical techniques, offering advantages like high magnification, large depth of focus, great resolution. Electrons generated from an electron gun enter a surface of sample and generate many low energy secondary electrons. The intensity of these secondary electrons is governed by the surface topography of the same. An image of the sample surface is therefore constructed by measuring secondary electron intensity as a function of the position of the scanning primary electron beam. EDX analysis is a useful tool widely used for chemical analysis. The intensity of backscattered electrons generated by electron bombardment can be correlated to the atomic number of the element within the sampling volume. Hence, qualitative elemental information can be revealed. The characteristic X-rays emitted from the sample serve as fingerprints and give elemental information for the samples, including semi-quantitative analysis, quantitative analysis, line profiling and spatial distribution of elements.
3. Results and Discussion
3.1. UV-Visible Studies
Figure 1 shows the UV-Visible spectra for zinc oxide and 5.0 wt% Mn-ZnO. These graphs show absorption peaks at 381.62 nm and 379 nm respectively. The strong absorption band in UV region for Zinc oxide and manganese doped zinc oxide can be attributed to the band edge absorption of wurtzite hexagonal ZnO, blue shift relative to its bulk 380 nm. The zinc oxide sample that is doped with Mn also shows the absorption band similar to zinc oxide. When Mn doped in ZnO nanoparticles, the position of the absorption spectra is shifted towards the lower wavelengths or known as blue-shifted which correlated to the change in the optical band gap value. Generally, blue-shifting in the bandgap was due to Mn doping in the ZnO nanoparticles with replacement of the Zn ions in the ZnO lattice by Mn ions. This indicates that the band gap of ZnO nanoparticles increases when doped with Mn. Furthermore, the blue-shifting of the band gap energy with increased Mn doping concentration can be defined as the separation in the energy between the top of the valence band and the unoccupied energy states in the conduction band [41].
3.2. FTIR Analysis
FTIR studies were performed in order to determine the presence of functional groups and chemical bonding, as well as to study the surface changes on the particles. These analyses can reveal the quality or consistency of sample. FTIR transmission spectra were obtained using a Bruker, Alpha T; Germany spectrometer from 500-4000 cm-1 using 2 cm-1 resolution. Various peaks corresponding to the main absorption bands can be seen from the FTIR spectrum on figure 2. The broad absorption bands at 3577 cm-1 and 3578 cm-1 represent the O-H stretching of the hydroxyl group. The band around 3100 cm-1 represents the O-H stretching [42]. The absorption bands observed between 1456 and 1330 cm-1 correspond to the asymmetric and symmetric stretching of the carbonyl group C=O. The small band at 879.97 and 628.104 cm-1 clearly indicate Zn-O stretching. From these studies, the stretching mode of undoped ZnO is at 628.104 cm-1. When doped with Mn, the absorption values were found to
Fig. 1. UV spectra of (a) pure and (b) Mn-doped ZnO
be blue-shifted at 618.8 and 595.30 cm-1 and were due to the Mn-O stretching and bending. Undoubtedly, this proves that the Zn-O-Zn network was perturbed by the presence of Mn in its environment as shown by the changes in the positions of the ZnO absorption bands [43].
4000 <000 UOO Ml 2600 JDOO 1HK 1000 -«SOO -«OOO 3SOO 3000 2WO 2000 1SOO IOOO
Wnvo number (cm '> Warn numbor (cm ')
(a) (b)
Fig. 2. FTIR Spectra (a) pure and (b) Mn doped ZnO
3.3. XRD Analysis
Figure 3 illustrates ZnO and manganese doped ZnO. (a) shows the XRD spectrum of ZnO. The eleven major peaks were seen at 23.3, 25.3, 31.7, 34.6, 36.2, 47.6, 56.5, 62.9, 67.9, 68.0 and 69.8 which can be assigned to diffraction from (-112), (310), (100), (002), (101), (102), (110), (103), (200), (112) and (201) planes respectively, which is in good agreement with the standard value JCPDS no, 36-1451. (b) shows the XRD spectrum of Mn doped ZnO. The twelve major peaks were seen at 23.3, 25.3, 31.7, 34.6, 36.2, 37.8, 47.6, 56.5, 62.9, 67.9, 68.0 and 69.8 which can be assigned to diffraction from (-112), (310), (100), (002), (101), (521), (102), (110), (103), (200), (112) and (201) planes respectively. The sharp intense peaks of ZnO confirm the well-defined crystalline nature of ZnO and diffraction peak can be indicative of a hexagonal wurtize structured zinc oxide. The average crystallite size can be estimated using the Debye-Scherrer formula:
2d = ^ <')
p cos 0
where, p is the full width at half maximum intensity [FWHM] corresponding to the diffraction angle 20 in radian, and A is the wave length of Cu-ka radiation. The average crystallite size for the prepared nanocomposite was found to be 30.587 nm for pure sample and 28.510 nm for doped sample.
(a) (b)
Fig. 3. XRD Pattern of (a) pure and (b) Mn doped ZnO
3.4. Particle Morphology
Figure 4(a) shows the SEM image of undoped ZnO nanoparticles and the corresponding EDX is given in 5(a). The SEM image reveals that the particles are spherical in shape and mono dispersed with sizes less than 40 nm. The SEM and EDX images of Mndoped ZnO are shown in 4(b) and 5(b) respectively. These clearly indicate the transformation of spherical rod shape with the particle size confinement with the result of Mndoping. in elemental analysis of zinc oxide, the peaks at 1.6 keV, 8.6 keV and 9.6 keV confirm the presence of zinc and the peak at 0.53 keV shows the presence of oxygen. The EDX spectra for the manganese-doped sample also confirmed the presence of zinc, oxygen and manganese. The peaks at 0.6 keV and 5.9 keV show the presence of manganese. The peak values at 1.6 keV and 8.6 keV, confirm the presence of zinc and the peak at 0.53 keV shows the presence of oxygen in the EDS spectra of manganese-doped ZnO.
(a) (b)
Fig. 4. SEM images of (a) pure and (b) Mn-doped ZnO nanoparticles
4. Conclusion
In summary, zinc oxide (ZnO) and the transition metal manganese doped at various percentages of zinc oxide was synthesized by using zinc acetate dihydrate as a precursor. The characterization of the samples was done using FTIR, UV-Visible spectrophotometer, XRD, SEM and EDX. The presence of functional groups and chemical bonding was determined by FTIR. The absorption peaks for all the synthesized samples were determined by UV-Visible spectrophotometry. The average crystallite sizes for all the samples were determined using XRD. The XRD peaks corresponded to the hexagonal wurtize structure. The SEM images were taken to determine the of the sample morphology. These analyses showed, the nanoparticles which were formed ranged from 75-90 nm. The EDX spectra were taken to determine the qualitative elemental information for zinc, oxygen and manganese in the synthesized particles.
Fig. 5. EDS Spectra of (a) pure and (b) Mn-doped ZnO
Acknowledgement
The author N. Joseph John acknowledges the University Grants Commission for providing financial support (No. F-MRP-4962/14 (MRP/UGC-SERO)).
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