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Structural, Magnetic and Gas Sensing Activity of Pure and Cr Doped In2O3 Thin Films Grown by Pulsed Laser Deposition

Veeraswamy YaraganiDepartment of Physics, Institute of Aeronautical Engineering, Dundigal, Hyderabad 500043, IndiaK. Hari PrasadDepartment of Physics, Institute of Aeronautical Engineering, Dundigal, Hyderabad 500043, IndiaK. Deva Arun KumarCollege of Engineering, Shibaura Institute of Technology, Saitama 337-8570, JapanPaolo MeleCollege of Engineering, Shibaura Institute of Technology, Saitama 337-8570, JapanArulanandam ChristyK.V. GunavathySultan AlomairyDepartment of Physics, College of Science, Taif University, P.O. Box 11099, Taif 21944, Saudi ArabiaM.S. Al-BuriahiDepartment of Physics, Sakarya University, 54100 Sakarya, Turkey
2021en
ABI

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Pure In2O3 and 6% Cr-doped In2O3 thin films were prepared on a silicon (Si) substrate by pulsed laser deposition technique. The obtained In2O3/In2O3:Cr thin films structural, morphological, optical, magnetic and gas sensing properties were briefly investigated. The X-ray diffraction results confirmed that the grown thin films are in single-phase cubic bixbyte structure with space group Ia-3. The SEM analysis showed the formation of agglomerated spherical shape morphology with the decreased average grain size for Cr doped In2O3 thin film compared to pure In2O3 film. It is observed that the Cr doped In2O3 thin film shows the lower band gap energy and that the corresponding transmittance is around 80%. The X-ray photoelectron spectroscopy measurements revealed that the presence of oxygen vacancy in the doped In2O3 film. These oxygen defects could play a significant role to enhance the sensing performance towards chemical species. In the magnetic hysteresis loop, it is clear that the prepared films confirm the ferromagnetic behaviour and the maximum saturation value of 39 emu/cc for Cr doped In2O3 film. NH3 gas sensing studies was also carried out at room temperature for both pure and Cr doped In2O3 films, and the obtained higher sensitivity is 182% for Cr doped In2O3, which is about nine times higher than for the pure In2O3 film due to the presence of defects on the doped film surface.

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