[39] Figure 2 Comparison of LIBS spectra of Si at atmospheric and

[39].Figure 2.Comparison of LIBS spectra of Si at atmospheric and 10-6 Palbociclib Phase 3 Torr. Reprinted from reference [38].Using a Nd:YLF laser with a 10 ns pulse duration, Dreyer et al. performed Inhibitors,Modulators,Libraries LIBS at varying reduced pressures on a hematite sample [39]. Figure 3 shows several LIBS spectra at varying pressures, focusing primarily on Ca and Mg lines. It can be observed in Figure 3 that as the surrounding pressure is decreased from 100 mbar to 10 mbar, a gradual increase in LIBS intensity is observed. Also, a maximum intensity occurs between 5 and 10 Torr, while pressures below 5 Torr resulted in a significant decrease in LIBS emission intensity. This significant decrease in emission intensity at very low pressures is also seen in work by Shu et al. comparing LIBS at lunar simulated condition of 5 �� 10?5 Pa (~10?7 Torr) and atmospheric conditions [16].

Inhibitors,Modulators,Libraries Dreyer et al. also observe a significant decrease in spectral intensity of ionic species between 7 and 5 Torr, suggesting a Inhibitors,Modulators,Libraries rapid decrease in electron density [39]. Dreyer et al. analyzed the LIBS spectra using a non-gated spectrometer. It is well known that a gated spectrometer yields higher quality LIBS spectra if the time is optimized; however, Dreyer et al. chose a non-gated spectrometer to remove some bias introduced in gated schemes when timing is optimized for one condition and is then carried through for all other conditions, which is a conundrum that other researchers have observed and dealt with in various ways.Figure 3.LIBS spectra of a geological sample (oolithic hematite) at various pressures. Reprinted from reference [39].

In addition to having an effect on the emission intensity and resolution, reduced pressures have also been shown to effect ablation from LIBS significantly. For example, Inhibitors,Modulators,Libraries in work performed by Vadillo et al. [40], the ablation from a laser plasma generated with a dye laser pumped by a XeCl laser with a 28 ns pulse width on iron or zinc samples showed a rather significant increase at 0.75 Torr compared to 750 Torr. At a laser fluence of 10 J/cm?2, Fe showed a 2.2-fold increase in ablation rate in 0.75 Batimastat Torr Ar compared to 750 Torr Ar atmosphere. A similar result was seen on ablation of Zn. With a laser fluence of approximately 3 J/cm?2, the Zn ablation rate was 3.7-fold greater in 0.75 Torr Ar compared to 750 Torr Ar atmosphere. It was also noted by Vadillo et al.

that the crater rims were free of deposited material after ablation at 0.75 Torr, while ablation at 750 Torr left craters with a visible ring of deposited material [40]. In other work by Vadillo et al., the 498.17 nm emission line from Ti(I) was monitored during laser ablation selleck inhibitor studies [41]. It was found that the emission intensity decreased with decreasing pressure. This result differs from other findings but this is likely due to the difference in which the experiments were conducted. Vadillo et al.

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