TY - JOUR A1 - Shelby, D. A1 - Merk, Sven A1 - Smith, B.W. A1 - Gornushkin, Igor B. A1 - Panne, Ulrich A1 - Omenetto, N. T1 - Temperature evaluation by simultaneous emission and saturated fluorescence measurements: A critical theoretical and experimental appraisal of the approach N2 - Temperature is one of the most important physical parameters of plasmas induced by a focused laser beam on solid targets, and its experimental evaluation has received considerable attention. An intriguing approach, first proposed by Kunze (H.-J. Kunze, Experimental check of local thermodynamic equilibrium in discharges, Appl. Opt., 25 (1986) 13–13.) as a check of the existence of local thermodynamic equilibrium, is based upon the simultaneous measurement of the thermal emission and the optically saturated fluorescence of the same selected atomic transition. The approach, whose appealing feature is that neither the calibration of the set-up nor the spontaneous radiative probability of the transitions is needed, has not yet been applied, to our knowledge, to analytical flames and plasmas. A critical discussion of the basic requirements for the application of the method, its advantages, and its experimental limitations, is therefore presented here. For our study, Ba+ transitions in a plasma formed by focusing a pulsed Nd:YAG laser (1064 nm) on a glass sample containing BaO are selected. At various delay times from the plasma initiation, a pulsed, excimer-pumped dye laser tuned at the center of two Ba transitions (6s ²S1/2 → 6p ²P°3/2; 455.403 nm and 6p ²P°1/2 → 6d ²S1/2; 452.493 nm) is used to enhance the populations of the excited levels (6p ²P°3/2 and 6d ²S1/2) above their thermal values. The measured ratio of the emission and direct line fluorescence signals observed at 614.171 nm (6p ²P°3/2 → 5d ²D5/2) and 489.997 nm (6d ²S1/2 → 6p ²P°3/2) is then related to the excitation temperature of the plasma. Our conclusion is that the approach, despite being indeed attractive and clever, does not seem to be easily applicable to flames and plasmas, in particular to transient and inhomogeneous plasmas such as those induced by lasers on solids. KW - Plasma temperature KW - Optically saturated fluorescence KW - Laser induced plasma KW - Barium ion emission KW - Emission/fluorescence ratio PY - 2013 U6 - https://doi.org/10.1016/j.sab.2013.09.002 SN - 0584-8547 SN - 0038-6987 VL - 89 SP - 50 EP - 59 PB - Elsevier B.V. CY - Amsterdam AN - OPUS4-30436 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Porizka, Pavel A1 - Klessen, Benjamin A1 - Kaiser, J. A1 - Gornushkin, Igor B. A1 - Panne, Ulrich A1 - Riedel, Jens T1 - High repetition rate laser-induced breakdown spectroscopy using acousto-optically gated detection N2 - This contribution introduces a new type of setup for fast sample analysis using laser-induced breakdown spectroscopy (LIBS). The novel design combines a high repetition rate laser (up to 50 kHz) as excitation source and an acousto-optical modulator (AOM) as a fast switch for temporally gating the detection of the emitted light. The plasma radiation is led through the active medium of the AOM where it is diffracted on the transient ultrasonic Bragg grid. The diffracted radiation is detected by a compact Czerny-Turner spectrometer equipped with a CCD line detector. Utilizing the new combination of high repetition rate lasers and AOM gated detection, rapid measurements with total integration times of only 10 ms resulted in a limit of detection (LOD) of 0.13 wt.% for magnesium in aluminum alloys. This short integration time corresponds to 100 analyses/s. Temporal gating of LIP radiation results in improved LODs and consecutively higher sensitivity of the LIBS setup. Therefore, an AOM could be beneficially utilized to temporally detect plasmas induced by high repetition rate lasers. The AOM in combination with miniaturized Czerny-Turner spectrometers equipped with CCD line detectors and small footprint diode pumped solid state lasers results in temporally gateable compact LIBS setups. KW - Laser Induced Breakdown Spectroscopy KW - LIBS KW - Aluminium KW - Charge coupled devices KW - Magnesium KW - Light diffraction PY - 2014 U6 - https://doi.org/10.1063/1.4890337 SN - 0034-6748 SN - 1089-7623 VL - 85 IS - 7 SP - 073104-1 - 073104-8 PB - American Institute of Physics CY - Melville, NY AN - OPUS4-31358 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Porizka, Pavel A1 - Demidov, Alexandr A1 - Kaiser, J. A1 - Keivanian, J. A1 - Gornushkin, Igor B. A1 - Panne, Ulrich A1 - Riedel, Jens T1 - Laser-induced breakdown spectroscopy for in situ qualitative and quantitative analysis of mineral ores N2 - In this work, the potential of laser-induced breakdown spectroscopy (LIBS) for discrimination and analysis of geological materials was examined. The research was focused on classification of mineral ores using their LIBS spectra prior to quantitative determination of copper. Quantitative analysis is not a trivial task in LIBS measurement because intensities of emission lines in laser-induced plasmas (LIP) are strongly affected by the sample matrix (matrix effect). To circumvent this effect, typically matrix-matched standards are used to obtain matrix-dependent calibration curves. If the sample set consists of a mixture of different matrices, even in this approach, the corresponding matrix has to be known prior to the downstream data analysis. For this categorization, the multielemental character of LIBS spectra can be of help. In this contribution, a principal component analysis (PCA) was employed on the measured data set to discriminate individual rocks as individual matrices against each other according to their overall elemental composition. Twenty-seven igneous rock samples were analyzed in the form of fine dust, classified and subsequently quantitatively analyzed. Two different LIBS setups in two laboratories were used to prove the reproducibility of classification and quantification. A superposition of partial calibration plots constructed from the individual clustered data displayed a large improvement in precision and accuracy compared to the calibration plot constructed from all ore samples. The classification of mineral samples with complex matrices can thus be recommended prior to LIBS system calibration and quantitative analysis. KW - Laser-induced breakdown spectroscopy KW - LIBS KW - Chemometrics KW - Principal component analysis KW - Geochemical analysis PY - 2014 U6 - https://doi.org/10.1016/j.sab.2014.08.027 SN - 0584-8547 SN - 0038-6987 VL - 101 SP - 155 EP - 163 PB - Elsevier CY - Amsterdam AN - OPUS4-32588 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Müller, Maike A1 - Gornushkin, Igor B. A1 - Florek, S. A1 - Mory, D. A1 - Panne, Ulrich T1 - Approach to Detection in Laser-Induced Breakdown Spectroscopy N2 - Gated detection with intensified detectors, e.g., ICCDs, is today the accepted approach for detection of plasma emission in laser-induced breakdown spectroscopy (LIBS). However, these systems are more cost-intensive and less robust than nonintensified CCDs. The objective of this paper is to compare, both theoretically and experimentally, the performance of an intensified (ICCD) and nonintensified (CCD) detectors for detection of plasma emission in LIBS. The CCD is used in combination with a mechanical chopper, which blocks the early continuum radiation from the plasma. The detectors are attached sequentially to an echelle spectrometer under the same experimental conditions. The laser plasma is induced on a series of steel samples under atmospheric conditions. Our results indicate that there is no substantial difference in the performance of the CCD and ICCD. Signal-to-noise ratios and limits of detection achieved with the CCD for Si, Ni, Cr, Mo, Cu, and V in steel are comparable or even better than those obtained with the ICCD. This result is further confirmed by simulation of the plasma emission signal and the corresponding response of the detectors in the limit of quantum (photon) noise. KW - LIBS KW - Detektorvergleich KW - ICCD CCD PY - 2007 U6 - https://doi.org/10.1021/ac0621470 SN - 0003-2700 SN - 1520-6882 VL - 79 IS - 12 SP - 4419 EP - 4426 PB - American Chemical Society CY - Washington, DC AN - OPUS4-15044 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Merk, Sven A1 - Shabanov, Sergej V. A1 - Gornushkin, Igor B. A1 - Panne, Ulrich T1 - Laser-induced plasma tomography by the Radon transform N2 - The Radon transform is tested as a method for reconstruction of the emissivity distribution of asymmetric laser induced plasmas. Two types of experiments were carried out. First, the plasma asymmetry is introduced via focusing the laser by a cylindrical lens to create plasma plumes elongated along the symmetry axis of the lens. Second, an asymmetric power distribution across the laser beam is created by reflecting the latter from a damaged mirror. Various effects on the quality of the plasma emissivity reconstructed by the Radon tomography method are investigated. The understanding of these effects appears to be essential to design a proper experimental setup to study LIBS plasmas by the Radon tomography method. It is demonstrated that the Radon tomography can successfully be used for experimental studies of asymmetric LIBS plasmas. KW - Radon transform KW - Laser induced plasma KW - LIBS KW - Plasma tomography PY - 2011 U6 - https://doi.org/10.1039/c1ja10187k SN - 0267-9477 SN - 1364-5544 VL - 26 SP - 2483 EP - 2492 PB - Royal Society of Chemistry CY - London AN - OPUS4-24889 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Merk, Sven A1 - Demidov, Alexandr A1 - Shelby, D. A1 - Gornushkin, Igor B. A1 - Panne, Ulrich A1 - Smith, B.W. A1 - Omenetto, N. T1 - Diagnostic of laser-induced plasma using Abel inversion and radiation modeling N2 - A method based on matching synthetic and experimental emissivity spectra was applied to spatially resolved measurements of a laser-induced plasma ignited in argon at atmospheric pressure. The experimental emissivity spectra were obtained by Abel inversion of intensity spectra measured from a thin plasma slice perpendicular to the plasma axis. The synthetic spectra were iteratively calculated from an equilibrium model of plasma radiation that included free free, free–bound, and bound–bound transitions. From both the experimental and synthetic emissivity spectra, spatial and temporal distributions of plasma temperature and number densities of plasma species (atoms, ions, and electrons) were obtained and compared. For the best-fit synthetic spectra, the temperature and number densities were read directly from the model; for experimental spectra, these parameters were obtained by traditional Boltzmann plot and Stark broadening methods. In both cases, the same spectroscopic data were used. Two approaches revealed a close agreement in electron number densities, but differences in plasma excitation temperatures and atom number densities. The trueness of the two methods was tested by the direct Abel transform that reconstructed the original intensity spectra for comparing them to the measured spectra. The comparison yielded a 9 and 13% difference between the reconstructed and experimental spectra for the numerical and traditional methods, respectively. It was thus demonstrated that the spectral fit method is capable of providing more accurate plasma diagnostics than the Boltzmann plot and Stark broadening methods. KW - Abel inversion KW - Laser-induced plasma KW - LIBS KW - Plasma spectrum analysis PY - 2013 U6 - https://doi.org/10.1366/12-06929 SN - 0003-7028 SN - 1943-3530 VL - 67 IS - 8 SP - 851 EP - 859 PB - Society for Applied Spectroscopy CY - Frederick, Md. AN - OPUS4-30433 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Matiaske, Anna-Maria A1 - Gornushkin, Igor B. A1 - Panne, Ulrich T1 - Double-pulse laser-induced breakdown spectroscopy for analysis of molten glass N2 - A mobile double-pulse laser-induced breakdown spectroscopy system for industrial environments is presented. Its capabilities as a process analytical technique for the recovery of metals from molten inorganic wastes are investigated. Using low-melting glass doped with different amounts of additives as a model system for recycling slags, the optimum number of shots, laser inter-pulse and acquisition delay times are optimized for solid and liquid (1200 °C) glass. Limits of detection from 7 ppm (Mn) to 194 ppm (Zn) are achieved working at a distance of 75 cm from the sample. To simplify the quantification of molten samples in an industrial furnace, the possibility is examined of using solid standards for analysis of molten material. KW - Laser-induced breakdown spectroscopy KW - LIBS KW - Double-pulse LIBS KW - Molten glass KW - Recycling PY - 2011 U6 - https://doi.org/10.1007/s00216-011-5165-2 SN - 1618-2642 SN - 1618-2650 VL - 402 IS - 8 SP - 2597 EP - 2606 PB - Springer CY - Berlin AN - OPUS4-23950 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Höhse, Marek A1 - Mory, D. A1 - Florek, S. A1 - Weritz, Friederike A1 - Gornushkin, Igor B. A1 - Panne, Ulrich T1 - A combined laser-induced breakdown and Raman spectroscopy Echelle system for elemental and molecular microanalysis N2 - Raman and laser-induced breakdown spectroscopy is integrated into a single system for molecular and elemental microanalyses. Both analyses are performed on the same ~ 0.002 mm² sample spot allowing the assessment of sample heterogeneity on a micrometric scale through mapping and scanning. The core of the spectrometer system is a novel high resolution dual arm Echelle spectrograph utilized for both techniques. In contrast to scanning Raman spectroscopy systems, the Echelle-Raman spectrograph provides a high resolution spectrum in a broad spectral range of 200-6000 cm- 1 without moving the dispersive element. The system displays comparable or better sensitivity and spectral resolution in comparison to a state-of-the-art scanning Raman microscope and allows short analysis times for both Raman and laser induced breakdown spectroscopy. The laser-induced breakdown spectroscopy performance of the system is characterized by ppm detection limits, high spectral resolving power (15,000), and broad spectral range (290-945 nm). The capability of the system is demonstrated with the mapping of heterogeneous mineral samples and layer by layer analysis of pigments revealing the advantages of combining the techniques in a single unified set-up. KW - LIBS KW - Raman KW - Echelle KW - Laser-induced breakdown spectroscopy KW - Hyphenated technique PY - 2009 U6 - https://doi.org/10.1016/j.sab.2009.09.004 SN - 0584-8547 SN - 0038-6987 VL - 64 IS - 11-12 SP - 1219 EP - 1227 PB - Elsevier CY - Amsterdam AN - OPUS4-20493 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Höhse, Marek A1 - Gornushkin, Igor B. A1 - Merk, Sven A1 - Panne, Ulrich T1 - Assessment of suitability of diode pumped solid state lasers for laser induced breakdown and Raman spectroscopy N2 - The potential of a diode pumped solid state (DPSS) laser for laser induced breakdown spectroscopy (LIBS) and Raman spectroscopy was investigated. The DPSS laser operating at repetition rates of 1 Hz–200 kHz, pulse energy of ~1 mJ, and pulse duration of ~20 ns was added to a conventional LIBS system equipped with the flashlamp-pumped Nd:YAG laser (10 Hz, 400 mJ, 6 ns) to directly compare the two laser systems. Despite the lower mass ablated per laser pulse (~several nanograms) and a weaker plasma, the total mass ablated per measurement interval (~1 s) and total emission signal were significantly higher than those obtained with the flashlamp pumped Nd:YAG laser. This resulted in the improved signal-to-noise ratio and better limits of detection (LOD). The best LODs were obtained for Cu, Cr and Ni in ultrapure standard iron samples, 0.7 ppm, 1 ppm and 5 ppm, correspondingly. The plasma from the DPSS laser was characterized in terms of its radiative properties, temperature, and shockwave propagation speed. The suitability of this laser for LIBS-Raman was demonstrated by mapping the elemental and molecular composition of a mineral sample. The results strongly imply that DPSS lasers are the promising source for LIBS, Raman, or combined LIBS-Raman spectroscopy. PY - 2011 U6 - https://doi.org/10.1039/c0ja00038h SN - 0267-9477 SN - 1364-5544 VL - 26 IS - 2 SP - 414 EP - 424 PB - Royal Society of Chemistry CY - London AN - OPUS4-22943 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Hoehse, M. A1 - Paul, Andrea A1 - Gornushkin, Igor B. A1 - Panne, Ulrich T1 - Multivariate classification of pigments and inks using combined Raman spectroscopy and LIBS N2 - The authenticity of objects and artifacts is often the focus of forensic analytic chemistry. In document fraud cases, the most important objective is to determine the origin of a particular ink. Here, we introduce a new approach which utilizes the combination of two analytical methods, namely Raman spectroscopy and laser-induced breakdown spectroscopy (LIBS). The methods provide complementary information on both molecular and elemental composition of samples. The potential of this hyphenation of spectroscopic methods is demonstrated for ten blue and black ink samples on white paper. LIBS and Raman spectra from different inks were fused into a single data matrix, and the number of different groups of inks was determined through multivariate analysis, i.e., principal component analysis, soft independent modelling of class analogy, partial least-squares discriminant analysis, and support vector machine. In all cases, the results obtained with the combined LIBS and Raman spectra were found to be superior to those obtained with the individual Raman or LIBS data sets. KW - Pigments KW - Raman KW - LIBS KW - Chemometrics PY - 2012 U6 - https://doi.org/10.1007/s00216-011-5287-6 SN - 1618-2642 SN - 1618-2650 VL - 402 IS - 4 SP - 1443 EP - 1450 PB - Springer CY - Berlin AN - OPUS4-25440 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER -