“…However, this assumption clearly contradicts the hydrodynamic hypotheses where the plasma plume pushes out the ambient gas by generating a shockwave. Hence there is no way for the energy to transfer from the gas to the plume and there is no possible electron-gas atom collision 23 until the plume pressure approximately reaches the ambient one. It remains that the most highly energetic species at the plasma plume front may still interact with the ambient gas and may induce its excitation or ionization.…”
Section: Dependence Of Excitation Temperature On Time Delay After mentioning
Time-resolved analysis of emission spectra, electron densities and excitation temperatures of Aluminum laser induced plasmas produced in argon, nitrogen and helium at different pressures have been studied experimentally. The plasma emission intensity is found to be strongly affected by the plume confinement and differs with the nature of the ambient gas and its pressure. Our observations show that both electron density and excitation temperature increase with the ambient gas pressure. In addition, Argon was found to produce the highest plasma density and temperature and Helium the lowest, while Nitrogen yields intermediate values.
“…However, this assumption clearly contradicts the hydrodynamic hypotheses where the plasma plume pushes out the ambient gas by generating a shockwave. Hence there is no way for the energy to transfer from the gas to the plume and there is no possible electron-gas atom collision 23 until the plume pressure approximately reaches the ambient one. It remains that the most highly energetic species at the plasma plume front may still interact with the ambient gas and may induce its excitation or ionization.…”
Section: Dependence Of Excitation Temperature On Time Delay After mentioning
Time-resolved analysis of emission spectra, electron densities and excitation temperatures of Aluminum laser induced plasmas produced in argon, nitrogen and helium at different pressures have been studied experimentally. The plasma emission intensity is found to be strongly affected by the plume confinement and differs with the nature of the ambient gas and its pressure. Our observations show that both electron density and excitation temperature increase with the ambient gas pressure. In addition, Argon was found to produce the highest plasma density and temperature and Helium the lowest, while Nitrogen yields intermediate values.
“…Rashid et al [34] reported the Cu plasma parameters generated by the fundamental, second and third harmonics of a Nd:YAG laser. [6] studied the expansion of a vapor plume ablated from an Al target into an argon gas at atmospheric pressure using time and spaceresolved emission spectroscopy and found plasma core with quite uniform distributions in electron density, temperature and electron number densities. Aragón and Aguilera [22] measured the local electron density in laser-induced plasma of three reference lines (Hα, Fe I and Si II) in air using a Nd:YAG laser and observed that the three lines was emitted from different regions of the plasma.…”
Section: Electron Temperature and Electron Number Density (End And Et)mentioning
confidence: 99%
“…The Pulsed laser-induced plasmas (LIPs) has a intensive application in material processing, thin film deposition, environmental monitoring, biomedical studies, military safety usage, art restoration/conservation and metal analysis, which is being produced after laser irradiance on the surface of metals and is of a great interest since last few decades [1][2][3][4][5][6][7][8][9][10][11]. In LIPS method, a micro-plasma is produced in nanosecond when highly intense laser pulse interacts with a target material; resultantly vaporization take place and thus plasma produced expand along the path of distribution in the form of vapor plume.…”
Silver (Ag) plasma generated by second harmonics (532 nm) using Nd:YAG laser has been investigated at 17.6 mJ and 88.6 mJ energy level. The spatial behavior of the END and Electron Temperature (ET) was measured at ambient air pressures at different energy level and distance ranging from 0-4.5 mm form the target metal. The ET's were found to be varies from 17895 K to 10593 K, while END was found to be 2.229 10 15 to 6.44 10 14 cm -3 and 1.76 10 16 to 1.893 10 15 cm -3 for 17.6 mJ and 88.6 mJ energy, respectively. The relationship of END and ET found directly related to laser irradiance, while they were inverse to the distance from the target material surface to laser beam source.
“…The sensitivity of LIBS can be significantly improved using the methods described above [19,20]. However, there are two drawbacks: one is the increased complexity of the LIBS setup, and the other is the increased cost of using more than one laser.…”
Hao, Z. Q.; Shen, M.; Xiong, W.; He, X. N.; Xie, Z. Q.; Gao, M.; Li, X. Y.; Zeng, X. Y.; and Lu, Yongfeng, "Accuracy improvement of quantitative analysis by spatial confinement in laser-induced breakdown spectroscopy" (2013
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