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Structural,optical and morphological properties of La,Cu co-doped SnO2 nanocrystals by co-precipitation method
Affiliation:1. Institute of Photonics, University of Eastern Finland, Joensuu 80101, Finland;2. Institute of Mechanics, Russian Academy of Sciences, Izhevsk 426067, Russia;3. Institute of Biophysics, Russian Academy of Sciences, Krasnoyarsk 660036, Russia;1. School of Materials Science and Engineering, Shanghai University, No. 99 Shangda Road, Baoshan District, Shanghai 200444, China;2. Instrumental Analysis and Research Center, Shanghai University, China;1. Jinan Engineering Vocational Technical College, Jinan, Shandong 250200, China;2. Qingdao University, Qingdao, Shandong 266071, China;1. Department of Physics, Sri Venkateswara University, Tirupati 517502, India;2. Department of BIN Fusion Technology & Department of Polymer-Nano Science and Technology, Chonbuk National University, Jeonju, Jeonbuk, Republic of Korea;3. Department of Chemistry and Chemical Institute for Functional Materials, Pusan National University, Busan 609-735, Republic of Korea
Abstract:Sn0.96?xLa0.04CuxO2 (0 ? x ? 0.03) nanocrystals have been successfully synthesized by employing a simple co-precipitation method. The crystal structure of the synthesized nanocrystals was found to be tetragonal rutile of tin oxide by using X-ray diffraction technique and was not affected by doping. The change in lattice parameters was discussed based on the secondary phase formation and presence of Cu2+/Cu3+ in Lasingle bondSnO2 lattice. The variation in size and shape of the nanocrystals by Cu-doping was discussed using scanning electron microscope. The chemical stoichiometry of Sn, Cu, La and O was confirmed by energy dispersive X-ray spectra. The best optical transparency and lower absorption observed at Sn0.97La0.02Cu0.01O2 nanocrystals seems to be optimal for industrial applications especially as transparent electrode. The initial blue shift of energy gap from 3.65 eV (Cu = 0%) to 3.78 eV (Cu = 1%) (ΔEg  0.13 eV) is due to the distortion in the crystal structure of the host compound and generation of defects. The red shift of energy gap after Cu = 1% is due to the charge-transfer transitions between the metal ions d-electrons and the SnO2 conduction or valence band. Lattice mode of SnO2 at 686 cm?1 in Sn0.98La0.02O2 nanocrystals and anti-symmetric Snsingle bondOsingle bondSn stretching mode of the surface bridging oxide around 634–642 cm?1 in Cu doped Sn0.98La0.02O2 nanocrystals was confirmed by Fourier transform infrared spectra.
Keywords:La  Co-precipitation  Optical property  FTIR spectra
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