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I assume you mean “lens-to-sample distance”. That will change the irradiance on sample (leading to a change in sampled mass). In addition to the distance, the position of the focus, either above or below the surface of the sample, is another parameter. Usually, the choice is to position the focus below the surface to avoid any excitation of the background gas above the surface. Several studies have shown a better stability of the signal when focused “inside the sample”.
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Yes. The optical properties will be different, and as a consequence the ablation and the emission. If your samples are known, it is easy to establish calibration curves for your elements of interest in a specific polymer matrix.
You can use LIBS on powders. It depends on your needs, you can pelletize such powder to increase the amount of material analyzed in one single laser shot.
Intensity I detected at a distance R is always ruled by the relation “I(R)=A/R2” where A is the area of the collector. Single-shot spectra of plasmas have been detected at several hundreds of meters. The sensitivity is increased if you optimize the detection timing and the optical coupling to the spectrometer.
You are right when you say that a major advantage is the direct solid sampling offered by LIBS. The comparison with LA-based methods (such as LA-ICP-MS or LA-ICP-OES) is often difficult because the ablation of followed in general by an ICP-based method. The ICP techniques are way more sensitive than LIBS because the plasma is well controlled and stable, in opposition to the LIBS plasma created during the sampling and only a transient event.
The use of pulse shaping has been explored for improving the emission of some elements in gases. This approach is promising, with the development of compact femtosecond lasers and should see more interest in the near future. Addressing the chemical bonds for ablation of polymers has also been explored and shows changes in the emission, but no analytical work has been done.
LIBS has been used for archeology but rather in laboratories than in the field. Then the advantages of LIBS can find a full application: no preparation, muti-element emission, elemental fingerprinting for databases.
You can find the information associated with your type of laser pulse (duration, spectrum) in publications. Some models can be evaluated. One reference is “Laser ablation threshold determination by photoelectric emission” by Beleznai et al. (Applied Physics A 69 S113)
Every spectral interference seen in a plasma technique could be seen in LIBS.
Yes. I don't know all of them but a search in Web of Science or Google Scholar will provide you some publications on these applications.
This is an area of interest for me since my PhD was on this subject. I believe LIBS can provide technological responses for the detection of pathogens. The analysis of the inorganic content has shown the way LIBS can be applied for pathogen identification. Furthermore, the need for data analysis of the rich spectrum is a crucial aspect in this application.
This question raises one of the needs for LIBS at the moment: a standardization of the experimental parameters. Usually, publications talk about spot sizes of 100 μm diameter. But other applications can go towards the micron and some to the millimeter.
LIBS for detection of energetic materials works. Several groups show that detection AND identification of the materials is possible.
The main question is: what is your need? Do you need a complete picture of the UV-Vis-NIR spectrum in a single laser shot or do you just want to analyze one or two elements. The echelle spectrometer is very interesting for the “exploratory” step of the analysis. Then , Czerny-Turner spectrometers are better suited for resolution and throughput in a quantitative step of the analysis.
You point it out yourself. I think more compact detectors adapted to LIBS (microsecond gates with low noise and nanosecond jitter) still need to be developed to apply LIBS in the field where iCCD cameras are not an option.
LIBS is not stochastic. Plasma physics and chemistry are modeled and understood in general. The main problem is to handle inhomogeneities of the sample and laser stability.