Synthesis, characterization and optical properties of zinc oxide nanoparticles
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Zinc oxide nanoparticles were synthesized using a simple precipitation method with zinc sulfate and sodium hydroxide as starting materials. The synthesized sample was calcined at different temperatures for 2 h. The samples were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM), energy dispersive spectroscopy (EDS), and proton-induced X-ray emission (PIXE) analysis. SEM images show various morphological changes of ZnO obtained by the above method. The average crystallite sizes of the samples were calculated from the full width at half maximum of XRD peaks by using Debye-Scherrer's formula and were found to be in the nanorange. EDS shows that the above route produced highly pure ZnO nanostructures. PIXE technique was used for trace elemental analysis of ZnO. The optical band gaps of various ZnO powders were calculated from UV-visible diffuse reflectance spectroscopic studies.
KeywordsNanostructures Semiconductors Chemical synthesis Catalytic properties Optical properties
Nanosized particles of semiconductor materials have gained much more interest in recent years due to their desirable properties and applications in different areas such as catalysts , sensors , photoelectron devices [3, 4], highly functional and effective devices . These nanomaterials have novel electronic, structural, and thermal properties which are of high scientific interests in basic and applied fields. Zinc oxide (ZnO) is a wide band gap semiconductor with an energy gap of 3.37 eV at room temperature. It has been used considerably for its catalytic, electrical, optoelectronic, and photochemical properties [6, 7, 8, 9]. ZnO nanostructures have a great advantage to apply to a catalytic reaction process due to their large surface area and high catalytic activity . Since zinc oxide shows different physical and chemical properties depending upon the morphology of nanostructures, not only various synthesis methods but also the physical and chemical properties of synthesized zinc oxide are to be investigated in terms of its morphology.
Many methods have been described in the literature for the production of ZnO nanostructures such as laser ablation , hydrothermal methods , electrochemical depositions , sol–gel method , chemical vapor deposition , thermal decomposition , and combustion method [17, 18]. Recently, ZnO nanoparticles were prepared by ultrasound , microwave-assisted combustion method , two-step mechanochemical-thermal synthesis , anodization , co-precipitation , and electrophoretic deposition .
Rodrigues-Paez et al. synthesized zinc oxide nanoparticles with different morphologies by controlling different parameters of the precipitation process such as solution concentration, pH, and washing medium . In the present study, ZnO nanostructures were synthesized using a simple precipitation method. Zinc sulfate heptahydrate and sodium hydroxide were used as precursors to formulate ZnO nanostructures. The prepared samples were characterized by X-ray diffraction (XRD) and scanning electron microscopy (SEM), and the purity of the sample was tested by energy dispersive spectroscopy (EDS) and proton-induced X-ray emission (PIXE) analysis. The band gap energies of the samples were calculated from diffuse reflectance spectroscopy. The morphology, crystallite size, and optical properties of ZnO nanostructures were investigated, and an attempt was made to correlate the optical properties of ZnO with morphology and crystallite size.
Zinc sulfate heptahydrate and sodium hydroxide were used in the experiments. All the chemicals used were of analytical reagent grade obtained from Merck (Mumbai, India), and deionized water is used for the preparation of solutions.
Synthesis of ZnO
To the aqueous solution of zinc sulfate, sodium hydroxide solution was added slowly dropwise in a molar ratio of 1:2 under vigorous stirring, and the stirring was continued for 12 h. The precipitate obtained was filtered and washed thoroughly with deionized water. The precipitate was dried in an oven at 100°C and ground to fine powder using agate mortar . The powder obtained from the above method was calcined at different temperatures such as 300°C, 500°C, 700°C, and 900°C for 2 h.
XRD and SEM
The compounds were characterized for their structure and morphology by XRD and SEM. The XRD patterns of the powdered samples were recorded using a Bruker D8 Advanced X-ray diffractometer (Bruker Optik GmbH, Ettlingen, Germany) with CuKα radiation (λ = 1.5418 Å, rated as 1.6 kW), and SEM images of the samples were taken using a Philips XL 30 ESEM scanning electron microscope (FEI-Philips Company, Hillsboro).
UV–vis diffuse reflectance spectroscopy
UV–vis spectroscopy was used to characterize the optical absorption properties of ZnO. The UV–vis absorption spectra of the samples were recorded in the wavelength range of 200 to 800 nm using a Shimadzu UV 3600 UV–vis-NIR spectrometer (Shimadzu Corporation, Kyoto, Japan) in diffuse reflectance mode using BaSO4 as reference. Spectra were recorded at room temperature, and the data were transformed through the Kubelka-Munk function .
Proton-induced X-ray emission
Finely powdered samples were mixed with pure graphite in the ratio of 1:1 (150 mg each), homogenized, and pressed into a 13-mm-diameter pellet. PIXE measurements have been carried out on a 3-MV horizontal pelletron accelerator at the Institute of Physics, Bhubaneswar . Proton beam was collimated to a diameter of 3 mm on the target. A Si(Li) detector was kept at 90° with respect to the beam direction. The detector has an active area of 30 mm2 with a beryllium window having a thickness of 12 μm and an energy resolution of 170 eV at 5.9 keV. Integrated charge on the sample was measured using a current integrator, which was connected to the target holder. The X-rays coming out of the chamber through a 95-μm Mylar window traveled through an air gap of 4 cm before entering the Si(Li) detector.
The targets were kept in the PIXE chamber at 45° to the beam. The Si(Li) detector is placed at 90° to the beam, and the beam current was kept in the range of 3 to 10 nA. Spectra were recorded using a Canberra MCA  (Canberra Industries, Meriden, CT, USA) and were transferred to a personal computer .
PIXE spectral analyses were carried out using GUPIX-95  software that provides nonlinear least-square fitting of the spectrum. The thick-target PIXE analysis was performed since the target was thick enough to stop the proton beam entirely. To check the adopted analysis procedure and input parameters, external standard method was adopted using the macrometer standards and other certified reference materials, and accordingly, the values were normalized. Further details about the analysis procedure can be obtained from our earlier references [28, 29].
Results and discussion
Average crystallite size of ZnO obtained from XRD using Equation 1
Calcination temperature (°C)
Crystallite size, D(nm)
where D is the crystallite size (nm), λ is the wavelength of incident X-ray (nm), β is the full width at half maximum, and θ is the diffraction angle.
SEM and EDS analysis
Diffuse reflectance analysis
Optical band gap of different ZnO samples calcined at different temperatures
Calcination temperature (°C)
Band gap (eV)
Concentration of various elements in ZnO nanoparticles
Statistical error (%)
ZnO nanoparticles were prepared using a simple precipitation method. The XRD and EDS analyses clearly indicate that highly pure ZnO is formed in the above method. SEM images of ZnO show that the morphology was changed with calcination temperature. PIXE analysis confirmed that the prepared material has a high purity and the presence of elements like Fe and Ti in trace level. The band gap of ZnO was decreased by an increase in calcination temperature, and the absorption maximum is also shifted to higher wavelengths.
SSK is indebted to the UGC Networking program, University of Hyderabad for providing instrumental facility to carry out the XRD and SEM analyses. The authors are thankful to the Institute of Physics for giving permission to carry out the PIXE analysis.
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Open AccessThis article is distributed under the terms of the Creative Commons Attribution 2.0 International License (https://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.