研究目的
The present work aims to grow high quality pure and Ag doped CdS nanocrystalline thin ?lms on glass substrates by a sol-gel spin coating method and to investigate the effect of Ag incorporation on physical and third-order nonlinear optical properties of CdS nanocrystalline thin ?lms. Moreover, based on the investigated properties, the study aims to evaluate the suitability of the produced ?lms for optoelectronic and nonlinear optical applications.
研究成果
In conclusion, the structural, vibrational, morphological, linear and non-linear optical properties of pure and Ag doped CdS nanocrystalline thin ?lms were investigated. The nanocrystalline structure of the grown ?lms was con?rmed by XRD studies, with estimated crystallite size of about 19–58 nm. A shift in the longitudinal optical phonon vibration peaks of the grown ?lms, as compared to the bulk CdS, was also noticed from Raman analysis, which con?rmed the formation of nano-size particles. SEM and AFM images of as-deposited ?lms demonstrated the formation of uniformly distributed spherical nanoparticles in the grown ?lms with relatively smooth surfaces. However, the roughness of the grown ?lms was found to increase with increasing Ag concentrations. Optical studies of the grown ?lms showed that transmittance of pure CdS ?lms is about 77% in the visible region and was found to decrease with increasing Ag concentrations. The band gap values of the grown ?lms were estimated and found to be in the range of 2.50 eV to 2.31 eV. A reduction in the band gap values of the doped ?lms was also noticed at high Ag concentrations. The linear refractive index of the grown ?lms was found to increase for the Ag concentrations 0.02 M and 0.03 M in the visible region. The values of nonlinear optical parameters such as v(3) and n2 were also calculated. The nonlinear optical constant was increased at 2.02 eV photon energy for Ag doping at both 0.02 M and 0.03 M concentrations. The ?ndings of the study demonstrate that the properties of the grown ?lms can be easily tuned by incorporating Ag into the CdS binary system. Furthermore, the values of nonlinear optical constants suggest that the grown ?lms are highly suitable for nonlinear optical device applications.
研究不足
The study does not explicitly mention limitations, but potential areas for optimization could include the control of Ag doping concentrations to further enhance the nonlinear optical properties and the investigation of other doping elements to compare their effects on the properties of CdS nanocrystalline thin ?lms.
1:Experimental Design and Method Selection:
Pure and Ag doped CdS nanocrystalline thin ?lms were grown using analytical grade cadmium acetate and thiourea as cadmium and sulpher sources, respectively. The chemicals used in this study were purchased from Sigma Aldrich. First, 1 M cadmium acetate and 1 M thiourea solutions were prepared in 2-methoxyethanol and stirred separately for 1 h at room temperature. The prepared solutions were then mixed together at 1:1 volume ratio and were stirred for 10 min. The freshly prepared solution was used for ?lms casting using a spin coater onto ultrasonically cleaned glass substrates. Each ?lm was coated up to ten times at 3000 rpm for 30 s. After each coating, ?lms were heated at 100(cid:2)C to remove the residual solvents from the samples. Incorporation of silver atoms into the ?lms was performed using ion exchange with different molar concentrations of silver acetate solution. Silver acetate aqueous solutions with concentrations of
2:01 M, 02 M and 03 M were prepared. Then, CdS ?lms were immersed in these solutions for 20 s and annealed at 400(cid:
2)C to remove water and organic residuals from the ?lms. Film thicknesses were estimated using an Alpha Step system and were found to be in the range of (cid:3) 200 nm. In this work, thicknesses of all samples were found to be nearly the same. The thicknesses of samples are listed in Table I. In addition, the prepared samples were characterized using various techniques, as discussed in the next section.
3:Sample Selection and Data Sources:
The prepared samples were characterized using different techniques. A Shimadzu (X-600 Japan) x-ray diffractometer with Cu-Ka radiation at 35 kV and 30 mA was used to record x-ray diffraction spectra of the prepared ?lms. The scan was performed with step size of
4:02 ? /s for the angular range (cid:
3) 5? -70? and using powder x-ray diffraction analysis. Raman spectra of Ag doped nanocrystalline thin ?lms at 300 K were measured in the range of 150–1500 cm(cid:2)1, using a THERMO SCIENTIFIC, DXR FT-RAMAN spectrometer joined with a microscope with optical setting speci?cation at grating range (cid:3) 5–3500 cm(cid:2)1, laser power 2 mW and using a 532 nm ?lter. The estimated resolution was
5:1 to 3 cm(cid:
2)1 and the size of the aperture was ?xed at 50 lm. The surface morphological studies of the prepared ?lms were analyzed using a scanning electron microscope (JSM 6360 LA, Japan). AFM was also used to study the grain size and roughness of the prepared samples using an NT-MDT atomic force microscope in non-contact mode. The transmittance, absorbance and re?ectance spectra of the ?lms in the range 200 nm to 2500 nm were recorded using a UV-Vis-Nir spectrophotometer (JASCO V-570).
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