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  • ا.م.د.احمد محمد شنو
  • Assist. Prof. Dr. Ahmed Mohammed Shano
  • رئيس قسم : تقنيات الاشعة والسونار
  • Head of the Department : Department of Radiology Techniques
  • دكتوراة علوم في الفيزياء - صلبة ومواد نانوية
  • PhD in Physics
  • drshano@bauc14.edu.iq
  • dr.ahmed.alaskari89@gmail.com
  • المقررات المكلف بها

    المقررات المكلف بها - 2
    القسم المرحلة الفصل رمز المقرر الوحدات توصيف المقرر
    تقنيات الاشعة والسونار المرحلة الثالثة فصل اول RA3-1-6 2 فيزياء الرنين المغناطيسي
    تقنيات الاشعة والسونار المرحلة الثالثة فصل ثاني RA3-2-6 2 فيزياء الامواج فوق الصوتية

    المحاضرات الالكترونية

    المحاضرات الالكترونية - 3
    العام المقرر القسم المرحلة المحاضرة
    2024-2025 فيزياء الرنين المغناطيسي تقنيات الاشعة والسونار المرحلة الثالثة محاضرة 3+4+5
    2024-2025 فيزياء الرنين المغناطيسي تقنيات الاشعة والسونار المرحلة الثالثة محاضرة 1+2
    2024-2025 فيزياء الامواج فوق الصوتية تقنيات الاشعة والسونار المرحلة الثالثة فيزياء الامواج فوق الصوتية (1-15)

    البحوث

    2015 International Journal of Thin Films Science and Technology
    Abstract: In this study, Ni0.92Co0.08O thin films with different molarities (0.05M, 0.1 M, 0.15M and 0.2 M) have been successfully deposited on glass substrates by chemical spray pyrolysis (CSP) technique at substrate temperature of (400 oC) and thickness of about 300 nm. The structural and optical properties of these films have been studied using XRD, AFM, and UV-Visible spectroscopy. The XRD results showed that all films are polycrystalline in nature with cubic structure and preferred orientation along (111) plane. The crystallite size was calculated using Scherrer formula and it is found that the 0.2M has maximum crystallite size (49.51nm). AFM results showed homogenous and smooth thin films. The absorbance and transmittance spectra have been recorded in the wavelength range of (300-900) nm in order to study the optical properties. The optical energy gap for allowed direct electronic transition was calculated using Tauc equation and First derivative of absorbance with respect to energy of photon. It is found that the band gap decreases when the molarity increases and the band gap values ranges between 3.60 eV and 3.54 eV for the prepared thin films. The Urbach energy increases as the molarity increases and the Urbach energy values range between 439 meV and 680 meV. The optical constants including (absorption coefficient, real and imaginary parts of dielectric constant) were also calculated as a function of photon energy. Refractive index and extinction coefficient for the prepared thin films were estimated as a function of wavelength.

    2015 International Letters of Chemistry, Physics and Astronomy
    In this work, nickel-cobalt oxide (Ni(1-x)CoxO) thin films, where x = 0, 4, 6 and 8 % have been successfully deposited on glass substrates by chemical spray pyrolysis (CSP) technique at substrate temperature of (400 °C) and thickness of about 300 nm. The structural and optical properties of these films have been studied using XRD, AFM, and UV-Visible spectroscopy. The XRD results showed that all films are polycrystalline in nature with cubic structure and preferred orientation along (111) plane. The crystallite size was calculated using Scherrer formula and it is found that the undoped NiO sample has maximum crystallite size (51.16 nm). AFM results showed homogenous and smooth thin films. The absorbance and transmittance spectra have been recorded in the wavelength range of (300-900) nm in order to study the optical properties. The optical energy gap for allowed direct electronic transition was calculated using Tauc equation. It is found that the band gap decreases as the Co-concentration increases and the band gap values were in the range of 3.58-3.66 eV and 3.58 eV for the prepared Nickel-Cobalt Oxide thin films. The Urbach energy increases as the Co-concentration increases and the Urbach. The optical constants including (absorption coefficient, real and imaginary parts of dielectric constant) were also calculated as a function of photon energy. Refractive index and extinction coefficient for Nickel- Cobalt Oxide thin films were estimated as a function of wavelength.

    2014 International Journal of Current Research
    In this work,NiO thin films at different molarities (0.05M, 0.1M, 0.15M and 0.2M)have been successfully deposited on glass substrates by chemical spray pyrolysis (CSP) technique at substrate temperature of (400 oC) and thickness of about 300 nm. The structural and optical properties of these films have been investigated using XRD, AFM, and UV-Visible spectroscopy. The XRD results showed that all films are polycrystalline in nature with cubic structure and preferred orientation along (111) plane. The crystallite size was calculated using Scherrer formula and it is found that the molarity 0.1M has maximum crystallite size (51.16nm). AFM images showed homogenous and smooth NiO thin films and the average grain size estimated from the AFM granularity report confirms the XRD results. The absorbance and transmittance spectra have been recorded in the wavelength range of (300-900) nm in order to study the optical properties.The optical energy gap for allowed direct electronic transition was calculated using Tauc equation. It is found that the band gap decreases when the molarity increases and the band gap values range between 3.71 eV and 3.59 eV for the preparedNiO thin films at different molarities. The Urbach energy increases as the molarity increases and the Urbach energy values range between 299 meV and 343 meV.The optical constants including (absorption coefficient, real and imaginary parts of dielectric constant) were also calculated as a function of photon energy. Refractive index and extinction coefficient for NiO thin films were estimated as a function of wavelength.

    2019 JOURNAL OF NANO- AND ELECTRONIC PHYSICS
    In this work, pure and copper mixed oxide PAni nanofiber thin films are successfully synthesized on silicon substrates by hydrothermal method and spin coating technique at room temperature with thickness of about 325 nm. The structural, surface morphological, optical and photoconductivity properties have been investigated. The XRD results showed that PAni films have crystalline nature, CuO and PAni/CuO nanostructure composites are monoclinic polycrystalline structure. The FESEM images of PAni clearly indicate that it has nanofiber-like structure, whereas the CuO film has sponge- like shape. The surface morphology analysis of PAni/CuO composite shows that nanofiber caped with inorganic material which is CuO is a core-shell structure. Optical characterization shows that the direct electronic transition is allowed in the energy gap. The values of energy gap for PAni nanofibers and CuO are 3.98 eV and 5.29 eV respectively. The spectral response of PAni nanofibers, CuO and PAni/CuO composite was studied. The values of responsivity and quantum efficiency of PAni/CuO composite are larger than those for pure PAni nanofibers. One can conclude that with mixing, the sensitivity is higher than that without mixing and is found to be 220 %. PAni/CuO composite exhibits fast rise time of 0.32 s with full time of 0.41 s, while slow rise time of 0.67 s and 0.38 s was respectively observed for PAni nanofibers and CuO with full time of 3.32 s and 1.19 s.

    2020 Journal of Nano- and Electronic Physics

    2023 AIP Conference Proceedings
    In this study, prepared the zirconia-alumina composites powders with weight ratios using aqueous aluminum nitrate and aqueous zirconia nitrate according to the molar fraction method of (A1) sample and using the molar fraction method in finding the weight ratios for each of the raw materials used in the preparation of the composites according to the following formula (ZrO2 (0.3-AI2O3(0.7)) and the ratio (2 from aluminum and 1 from zirconium) is from the raw materials, and the second sample (A2) according to the traditional ceramic method of direct quantities and is in a ratio (1 to 1) from the raw materials and by the method of common chemical precipitation and using dilute ammonia with a concentration of 30-33 The acidic function=10 as a strong base for precipitation to obtain the hydroxides of the materials and the sintered primary sintering at Heat of 600 oC for 4 hours and then a final sintering at 1300 oC for four hours. X-ray diffraction pattern spectroscopy (XRD-patterns) of the compound powders prepared at a temperature of (1300 oC) showed that the first sample was at the weight ratio A1 of the primary alumina-button superimposed and formed with two different phases, phase α-AI2O3 and orthogonal phase of zirconia t-zro2. As for the second sample the predominant phase is the orthogonal phase of zirconia t-zro2 with some phases of alumina. Fourier transformations of the infrared spectrum (FTIR) of the powders prepared at a temperature of (1300 oC) showed that they formed the required phases and were pure due to the high sintering temperature and were within the numbers less than (1000cm−1).




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