Abstract:Laser-induced plasma from an aluminum target in one-atmosphere argon background has been investigated with ablation using nanosecond ultraviolet (UV: 355 nm) or infrared (IR: 1064 nm) laser pulses. Time- and space-resolved emission spectroscopy was used as a diagnostics tool to have access to the plasma parameters during its propagation into the background, such as optical emission intensity, electron density, and temperature. The specific feature of nanosecond laser ablation is that the pulse duration is sign… Show more
“…The used experimental setup is described in detail elsewhere [18][19][20][21][22], we provide here its brief description. Two Q-switched Nd:YAG lasers were used for ablation with IR (1064 nm) or UV (266 nm) radiation, with a repetition rate of 10 Hz and a pulse duration of 5 ns.…”
Section: Experimental Setup Samples Measurement Protocol and Data Tmentioning
confidence: 99%
“…Quite different properties can be expected for ablation plumes induced on the surface of these two types of materials, which obviously leads to specific considerations when optimizing experimental conditions for LIBS analyses. Up to now, even though extensive studies have been devoted to the characterization of plasma induced on metallic samples [13][14][15][16][17][18][19][20][21][22], the investigation of the plasma induced on the surface of dielectric materials remains rare. Main interests were focused on the influence of the ablation wavelength on the analytical performance of the induced plasma [23,24].…”
“…The used experimental setup is described in detail elsewhere [18][19][20][21][22], we provide here its brief description. Two Q-switched Nd:YAG lasers were used for ablation with IR (1064 nm) or UV (266 nm) radiation, with a repetition rate of 10 Hz and a pulse duration of 5 ns.…”
Section: Experimental Setup Samples Measurement Protocol and Data Tmentioning
confidence: 99%
“…Quite different properties can be expected for ablation plumes induced on the surface of these two types of materials, which obviously leads to specific considerations when optimizing experimental conditions for LIBS analyses. Up to now, even though extensive studies have been devoted to the characterization of plasma induced on metallic samples [13][14][15][16][17][18][19][20][21][22], the investigation of the plasma induced on the surface of dielectric materials remains rare. Main interests were focused on the influence of the ablation wavelength on the analytical performance of the induced plasma [23,24].…”
“…Our previous works show that such fluence is already high enough, especially for an IR pulse, to induce a strong post-ablation interaction leading to a strong plasma shielding. 4 The behaviors of the plasmas induced by the short pulse and the long pulse will first be compared in detail over the delay interval between 500 ns and 2 ls. The observations clearly show different behaviors between the plasmas produced by these two types of pulse.…”
Section: Effect Of Pulse Duration On the Property Of The Plasma mentioning
We studied the behavior of the plasma induced by a nanosecond infrared (1064 nm) laser pulse on a metallic target (Al) during its propagation into argon ambient gas at the atmospheric pressure and especially over the delay interval ranging from several hundred nanoseconds to several microseconds. In such interval, the plasma is particularly interesting as a spectroscopic emission source for laser-induced plasma spectroscopy (LIBS). We show a convoluted effect between laser fluence and pulse duration on the structure and the emission property of the plasma. With a relatively high fluence of about 160 J/cm2 where a strong plasma shielding effect is observed, a short pulse of about 4 ns duration is shown to be significantly more efficient to excite the optical emission from the ablation vapor than a long pulse of about 25 ns duration. While with a lower fluence of about 65 J/cm2, a significantly more efficient excitation is observed with the long pulse. We interpret our observations by considering the post-ablation interaction between the generated plume and the tailing part of the laser pulse. We demonstrate that the ionization of the layer of ambient gas surrounding the ablation vapor plays an important role in plasma shielding. Such ionization is the consequence of laser-supported absorption wave and directly dependent on the laser fluence and the pulse duration. Further observations of the structure of the generated plume in its early stage of expansion support our explanations.
“…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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