scholarly journals Spectroscopic Analysis of CdO1-X: SnX Plasma Produced by Nd:YAG Laser

2020 ◽  
pp. 1665-1671
Author(s):  
Madyan A. Khalaf ◽  
Baida M. Ahmed ◽  
Kadhim A. Aadim
Keyword(s):  
Electron Temperature ◽  
Spectroscopic Analysis ◽  
Outcome Measure ◽  
Focal Length ◽  
Debye Length ◽  
Optical Emission ◽  
Plasma Parameters ◽  
Optical Emission Spectrum ◽  
Mixing Ratios ◽  
Line Intensities

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.

scholarly journals Spectroscopic Diagnosis of the CdO:CoO Plasma Produced by Nd:YAG Laser

2021 ◽  
pp. 2948-2955
Author(s):  
Maryam M. Shehab ◽  
Kadhim A. Aadim
Keyword(s):  
Electron Temperature ◽  
Nd:Yag Laser ◽  
Laser Energy ◽  
Focal Length ◽  
Optical Emission ◽  
Ratio Method ◽  
Plasma Parameters ◽  
Optical Emission Spectrum ◽  
Boltzmann Plot ◽  
Laser Induced Plasma

      In this paper, the optical emission spectrum (OES) technique was used to analyze the spectrum resulting from the (CdO:CoO)  plasma in air, produced by Nd:YAG laser with λ=1064 nm, τ=10 ns, a focal length of 10 cm, and a range of energy of 200-500 mJ. We identified laser-induced plasma parameters such as electron temperature (Te) using Boltzmann plot method, density of electron (ne), length of Debye (λD), frequency of plasma (fp), and number of Debye (ND), using two-Line-Ratio method. At a mixing ratio of X= 0.5, the (CdO:CoO) plasma spectrum was recorded for different energies. The results of plasma parameters caused by laser showed that, with the increase in laser energy, the values of Te, ne and fp were increased, while the value of λD was decreased. The calculated electron temperature value was in the range of 0.449-0.619 eV at ratio X=0.5

scholarly journals Optical Emission Spectroscopic Analysis of Plasma Parameters in Cadmium by Nd: YAG laser Technique

2021 ◽  
Vol 2114 (1) ◽  
pp. 012049
Author(s):  
Uday H. Tawfeeq ◽  
Ahmed K. Abbas ◽  
Kadhim A. Aadim
Keyword(s):  
Laser Pulse ◽  
Atmospheric Pressure ◽  
Spectroscopic Analysis ◽  
Debye Length ◽  
Optical Emission ◽  
Plasma Electron ◽  
Laser Technique ◽  
Plasma Parameters ◽  
Yag Laser ◽  
Emission Spectroscopic Analysis

Abstract In this work, optical emission spectroscopy (OES) was used to estimate the parameters of plasma electron temperature (Te), electron density (ne), plasma frequency (fp), Debye length (λD), and Debye number (ND). Understanding how an energy pulsed laser affects these variables is also important. Irradiation of pure cadmium using an Nd: YAG laser pulse with a wavelength(1064)nm and energy ranging from (200-600)millijoules, of frequency (6) Hz. The spectrum of laser-induced plasma was detected under atmospheric pressure. It was discovered that when the energy of the laser pulse rises, the intensity of the CdI and CdII lines increases.

scholarly journals Synthesis Emission Spectra of (LIPS) Technique for Cu, Ag Nanoparticles and their Antibacterial Activity

2021 ◽  
Vol 32 (3) ◽  
pp. 49
Author(s):  
Hadeel K. Nasif ◽  
Baida M. Ahmed ◽  
Kadhim A. Aadim
Keyword(s):  
Laser Ablation ◽  
Focal Length ◽  
Emission Spectra ◽  
Optical Emission ◽  
Resistant Bacteria ◽  
Distilled Water ◽  
Ag Nps ◽  
Plasma Parameters ◽  
Optical Emission Spectrum ◽  
Constant Frequency

A spectroscope presents the optical emission spectroscopy (OES) technique on laser-produced copper and silver plasmas. The optical emission spectrum technique was used to analyzes the spectrum arising from the Cu, Ag Laser Nd: YAG plasmas with a wavelength of (1064) nm, a span of (10) ns, and a focal length of (10) cm in the energy range (300-800) mJ. The electron temperature (Te) was determined while the Saha-Boltzmann equation was used to measure the electron density (ne). Other plasma parameters, (λD), (fp), (ND), were also measured. For various energies, the plasma spectrum was registered copper and silver. Q-switched Nd: YAG liquid laser ablation technique (PLAL) was used to produce nanoparticles (NPs), silver, and copper particles using distilled water at room temperature at different energies (300-600-800) mJ. With a constant wavelength (1064nm). At a constant frequency (6Hz), 300 laser pulses were used to ablate the target placed in distilled water to study the effect of these materials in inhibiting bacteria. Bacteria were used (Staphylococcus). This study showed that (Ag-NPs) and (Cu-NPs) that are synthesized by laser ablation have a great effect on Staphylococcus (antibiotic-resistant) bacteria.

Effect of Current on Plasma Parameters Resulting from the Wires-Exploding Technique of Copper Material

2020 ◽  
pp. 110-113
Keyword(s):  
Electron Temperature ◽  
Electron Density ◽  
Optical Emission ◽  
Plasma Electron ◽  
Stark Broadening ◽  
Number Density ◽  
Hydrogen Atoms ◽  
Plasma Parameters ◽  
Optical Emission Spectrum ◽  
Copper Material

In this research the diagnostic of optical emission spectroscopy from exploding copper wires have done for different current. By using Boltzman plot can be calculated the plasma electron temperature , and by using Stark broadening can be evaluated the electron density for different current of (75, 100 and 150)A with diameter 0.25 mm in deionized water. It was observed that the electron density decrease with an increasing the current from 75 A to 150 A while the electron temperatures increase for the same current. The plasma has a peak 652 nm corresponding to Hα line for .hydrogen .atoms which obtained from .optical emission spectrum (OES), the peaks belong to atomic copper lines. The plasma electron temperature related with emission line intensity and number .density with the formed copper nanoparticles size was studied.

scholarly journals Influence of Gas Type on the Laser Produced Graphite Plasma

2021 ◽  
Vol 2114 (1) ◽  
pp. 012030
Author(s):  
H Adil A Alazawi ◽  
Q Adnan Abass
Keyword(s):  
Electron Temperature ◽  
Electron Density ◽  
Plasma Frequency ◽  
Laser Energy ◽  
Debye Length ◽  
Optical Emission ◽  
Plasma Parameters ◽  
Pulse Laser Energy ◽  
Electron Density Increase ◽  
Ionic Emission

Abstract Plasma graphite creation by a pulsed Nd: YAG laser with a wavelength of 1064nm to a target in vacuum in two cases (Argon, Air) with varied gas pressures and the resulting spectrum was diagnosed using optical emission spectroscopy for the wavelength range 320-740nm electron temperature Te and electron density ne Debye lengthλD , and plasma frequency f p were calculated. The results showed that increasing the pulse laser energy causes all plasma parameters of both gases under study to increase, as well as a rise in the emission line intensity. The ionization energy of target atoms determines the presence of an element’s atomic and ionic emission lines in the emission spectrum, increase in pressure decreases the electron temperature, and Debye length, also plasma frequency and electron density increase, as it has been proven that the type of gas does not affect the properties of plasma.

scholarly journals COMPARISON STUDY BETWEEN SPECTROSCOPIC ANALYSIS FOR (ZN,SN) PLASMA BY LIBS

2021 ◽  
Vol 03 (02) ◽  
pp. 52-61
Author(s):  
Hadeel K. NASIF ◽  
Kadhim A. AADIM ◽  
Baida M. AHMED
Keyword(s):  
Emission Spectroscopy ◽  
Optical Emission Spectroscopy ◽  
Spectroscopic Analysis ◽  
Focal Length ◽  
Line Strength ◽  
Pulsed Laser ◽  
Optical Emission ◽  
Comparison Study ◽  
Plasma Parameters ◽  
Strength Formula

this article a spectroscopic research on laser-produced Tin and Zinc plasmas using the optical emission spectroscopy (OES) technique. Plasmas can be produced from a solid tin and zinc targets irradiated with a pulsed laser in room environments. The spectrum is recorded for the Sn, Zn laser plasma Nd: YAG with a wavelength of (1064) nm, a duration of (9) ns, and a frequency of (6) Hz and a focal length of (10) cm within the energy range (300-800)mj. By using the ratio line strength formula, the electron temperature (Te) can be calculated and the result is for Zinc (Zn) plasma (2.11 ev) and tin (Sn) plasma (1,227 ev). The Saha-Boltzmann equation will be used to calculate electron density (ne) in this method and the values for zinc (Zn) (3.3 cm-3)and tin (Sn) (2.1 cm-3). The plasma parameters, such as plasma (fp), Debye duration (λD), and Debye number (ND), were calculated in the proposed document.

scholarly journals Spectroscopic study the plasma parameters for Pb doped CuO prepared by pulse Nd:YAG laser deposition

2018 ◽  
Vol 16 (38) ◽  
pp. 1-9
Author(s):  
Kadhim A Aadim
Keyword(s):  
Spectroscopic Study ◽  
Electron Temperature ◽  
Optical Transmission ◽  
Optical Emission Spectroscopy ◽  
Plasma Frequency ◽  
Debye Length ◽  
Optical Emission ◽  
Spectroscopy Technique ◽  
Transmission Method ◽  
Plasma Parameters

In this work, plasma parameters such as, the electron temperature )Te(, electron density ne, plasma frequency )fp(, Debye length )λD(and Debye number )ND), have been studied using optical emission spectroscopy technique. The spectrum of plasma with different values of energy, Pb doped CuO at different percentage (X=0.6, 0.7, 0.8) were recorded. The spectroscopic study for these mixing under vacuum with pressure down to P=2.5×10-2 mbar. The results of electron temperature for X=0.6 range (1.072-1.166) eV, for X=0.7 the Te range (1.024-0.855) eV and X=0.8 the Te is (1.033-0.921) eV. Optical properties of CuO:Pb thin films were determined through the optical transmission method using ultraviolet visible spectrophotometer within the range (190 – 1100) nm.

Measurement of Plasma Parameters of Fe-Lines in Lipstick Using Laser-Induced Breakdown Spectroscopy

2021 ◽  
Vol 19 (10) ◽  
pp. 01-07
Author(s):  
M.H. Asmaa ◽  
Sami A. Habana
Keyword(s):  
Electron Temperature ◽  
Debye Length ◽  
Nuclear Data ◽  
Laser Induced Breakdown Spectroscopy ◽  
Current Investigation ◽  
Plasma Parameters ◽  
Data Set ◽  
Breakdown Spectroscopy ◽  
Laser Induced Breakdown ◽  
Business Sectors

Electron thickness and temperature of laser prompted Iron plasma boundaries, among different boundaries, were estimated. Plasma was delivered through the connection of high pinnacle power Nd: YAG laser at the key frequency of 1064 nm with a pellet target contains a limited quantity of lipstick from nearby business sectors. Lines from Fe II at 238.502 nm, Fe II at 254.904 nm, Fe II at 262.370 nm, Fe II at 286.545 nm and Fe I at 349.779 nm were utilized to assess the plasma boundaries. The current investigation was completed to assess electron temperature (Te), electron thickness (ne), plasma recurrence, Debye length and Debye number (ND). Laser-incited breakdown spectroscopy LIBS method was used for examining and deciding ghastly discharge lines. ID of change lines from all spectra was completed by contrasting ghostly lines and NIST nuclear data set.

scholarly journals Machine Learning Prediction of Electron Density and Temperature from Optical Emission Spectroscopy in Nitrogen Plasma

Coatings ◽  
2021 ◽  
Vol 11 (10) ◽  
pp. 1221
Author(s):  
Jun-Hyoung Park ◽  
Ji-Ho Cho ◽  
Jung-Sik Yoon ◽  
Jung-Ho Song
Keyword(s):  
Machine Learning ◽  
Electron Temperature ◽  
Real Time ◽  
Electron Density ◽  
Emission Spectroscopy ◽  
Optical Emission Spectroscopy ◽  
Optical Emission ◽  
Plasma Parameters ◽  
Plasma Nitridation

We present a non-invasive approach for monitoring plasma parameters such as the electron temperature and density inside a radio-frequency (RF) plasma nitridation device using optical emission spectroscopy (OES) in conjunction with multivariate data analysis. Instead of relying on a theoretical model of the plasma emission to extract plasma parameters from the OES, an empirical correlation was established on the basis of simultaneous OES and other diagnostics. Additionally, we developed a machine learning (ML)-based virtual metrology model for real-time Te and ne monitoring in plasma nitridation processes using an in situ OES sensor. The results showed that the prediction accuracy of electron density was 97% and that of electron temperature was 90%. This method is especially useful in plasma processing because it provides in-situ and real-time analysis without disturbing the plasma or interfering with the process.

scholarly journals Spectroscopic Analysis of DC-Nitrogen Plasma Produced using Copper Electrodes

2021 ◽  
pp. 3560-3569
Author(s):  
Ala F. Ahmed ◽  
Ali A. Yousef
Keyword(s):  
Debye Length ◽  
Target Material ◽  
Optical Emission ◽  
Nitrogen Plasma ◽  
Molecular Spectra ◽  
Stark Broadening ◽  
Plasma Parameters ◽  
Working Pressure ◽  
Copper Electrodes ◽  
Copper Material

      This study shows the effects of copper material electrode, applied voltage, and different pressure values on electrical discharge plasma. The purpose of the work is the application of the spectral analysis method to obtain accurate results of nitrogen plasma parameters. By using the optical emission spectroscopy (OES), many N2 molecular spectra peaks appeared in the range from 300 to 480 nm. Also, some additional peaks were recorded, corresponding to atomic and ionic lines for nitrogen, target material, and hydrogen, in all samples. The electron density (ne) was calculated from the measurement of Stark broadening effect, which was found to decrease with increasing pressure from 0.1 mbar to 0.8 mbar. The higher emission intensities occurred at 0.2 mbar working pressure and were reduced with higher pressure. The vibrational temperature (Tvib) for N2 increased from 0.17 to 0.33 eV with increasing the pressure from 0.15 mbar to 0.2 mbar, then decreased to 0.25 eV with increasing the pressure to 0.8 mbar. Other plasma parameters were studied, which are electron temperature (Te), plasma frequency of electron ( ), and Debye length (λD).

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