In this work, the optical emission spectrum technique was used to analyze the spectrum resulting from the CdO:Sn plasma produced by laser Nd:YAG with a wavelength of (1064) nm, duration of (9) ns, and a focal length of (10) cm in the range of energy of 500-800 mJ. The electron temperature (Te) was calculated using the in ratio line intensities method, while the electron density (ne) was calculated using Saha-Boltzmann equation. Also, other plasma parameters were calculated, such as plasma (fp), Debye length (λD) and Debye number (ND). At mixing ratios of X=0.1, 0.3 and 0.5, the CdO1-X :SnX plasma spectrum was recorded for different energies. The changes in electron temperature and the densities were studied as a function of the laser energies. Outcome measure value of the electron temperature at the ratio of  X = 0.1 was (1.079-1.054) eV, while at  X=0.3 the Te range was (0.952- 0.921) eV and at X=0.5 it was (0.928-0.906) eV.

In this work, we study the effect of doping Sn on the structural and optical properties of pure cadmium oxide films at different concentrations of Tin (Sn) (X=0.1,0.3 and 0.5) .The films prepared by using the laser-induced plasma at wavelength of laser 1064 nm and duration 9 ns under pressure reached to 2.5×10-2 mbar. The results of X-ray diffraction tests showed that the all prepared films  are polycrystalline. As for the topography of the films surface, it was measured using AFM , where the results showed that the grain size increases with an increase in the percentage of doping  in addition to an increase in the average roughness. The optical properties of all films have also been studied through the absorbance spectrum of the range  of  the wavelength (350-1100) nm, where the optical energy gap was direct transitions it was found that the value of the optical energy gap increased with increasing the doping.

In this study, plasma was generated from laser-induced plasma and the parameters of the plasma were analysed using the optical emission spectroscopy technique. A 1064 nm wavelength Nd:YAG laser with a frequency of 6 Hz within a 9 ns timeframe, was used. The ratio between two spectral lines was used to calculate the temperature of the electron (T e), while the Saha-Boltzmann method was used to find the density of electrons (n e) for wavelengths between 170-670 nm, by changing the laser energies within the 400-900 mJ region. The remaining plasma parameters were also calculated. These included the Debye length ( D), the plasma frequency (ω p) and the number of atoms within the Debye sphere (N D). Three relationship diagrams illustrate the relationship between laser energy change and the plasma parameter collection. The highest possible electron temperature is 1.453 eV, while the lowest possible temperature is 1.216 eV. The upper limit of the electron density has reached 6.5 × 10 18 cm-3 , and its lowest value is 1.7 × 10 18 cm-3 .

High-intensity laser-produced plasma has been extensively investigated in many studies. In this demonstration, a new spectral range was observed in the resulted spectra from the laser-plasma interaction, which opens up new discussions for new light source generation. Moreover, the characterizations of plasma have been improved through the interaction process of laser-plasma. Three types of laser were incorporated in the measurements, continuous-wave CW He-Ne laser, CW diode green laser, pulse Nd: YAG laser. As the plasma system, DC glow discharge plasma under the vacuum chamber was considered in this research. The plasma spectral peaks were evaluated, where they refer to Nitrogen gas. The results indicated that the plasma intensity increased from several thousands to several tens of thousands through the process of interaction of the Nd: YAG laser with the plasma. This increase in the intensity of the plasma as laser intensity increased occurs regardless of laser wavelength involved in the interaction or not. According to laser-plasma interaction, the so-called full width at half maximum FWHM of the highest peak in the plasma spectrum was broadened from 1.43 to 2.73. Considering the equation of plasma density computing, the plasma density was increased from 1.07× 1018 to 2.05× 1018   cm-3 with increasing FWHM. As a result of the interaction, the electron temperature of plasma was increased from 0.176 to 0.782 eV. It was also noticed that the position of the highest peak in the plasma spectrum depends on the interacted laser wavelength.

In this research, Argon gas was used to generate atmospheric plasma in the manufacture of platinum nanomaterials, to study the resultant plasma spectrum and to calculate the cellular toxicity of those manufactured nanomaterials. This research is keen on the generation of nonthermal atmospheric pressure plasma using aqueous platinum salts (H2PtCl6 6H2O) with different concentrations and exposure of cold plasma with a different time period used to produce platinum nanoparticles, to ensure typical preparation of nanoparticles. Visible UV and X-rays were performed for this purpose, and the diameter of the system probe was (1[Formula: see text]mm) with the Argon gas flow of 2.5[Formula: see text]min/L to prepare the platinum nanoparticles, and spectroscopic study of plasma parameter including, electron temperature, electron density, Debye length and plasma frequency, were computed using spectral analysis techniques. The effect of nanoparticles on natural lymphocytes was studied to calculate cytotoxicity and the greatest proportion was at the concentration of 100% nanoparticle platinum is 37.4%. The study results revealed that cold in the atmosphere is a promising technology when used in the production of nanoparticle materials which can be used for many industrial and medical applications.