TY - JOUR A1 - Glaus, Reto A1 - Gornushkin, Igor B. A1 - Nagli, L. T1 - Stimulated emission in aluminum laser-induced plasma: an experimental study JF - Applied Optics N2 - The stimulated emission (SE) in aluminum laser-induced plasma pumped in resonance with the 3s23p − 3s24s aluminum transition at 266.04 nm is investigated experimentally. It is shown that the population Inversion between the 3s23p and 3s24s states can be created by weak pumping at several microjoule to millijoule pulse energies and result in high gain. The intensity of the SE at 396.15 nm is related to the number density of Al Atoms via absorption measurements. It is found that the SE in forward and backward directions with respect to the pumping laser is different in terms of the line shape and intensity that is attributed to inhomogeneity in a gain coefficient across the plasma plume. KW - Spectroscopy KW - Lasers KW - Laser induced breakdown PY - 2017 DO - https://doi.org/10.1364/AO.56.003699 SN - 1559-128X SN - 0003-6935 SN - 1539-4522 VL - 56 IS - 13 SP - 3699 EP - 3702 PB - Optical Society of America CY - Washington, DC, USA AN - OPUS4-40134 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Glaus, Reto A1 - Nagli, L. A1 - Gornushkin, Igor B. T1 - Stimulated emission in aluminum laser-induced JF - Applied Optics N2 - The stimulated emission (SE) in aluminum laser-induced plasma pumped in resonance with the 3s²3p-3s²4s aluminum transition at 266.04 nm is modeled. A collisional-radiative plasma model based on kinetic equations is proposed to explain the creation of the population inversion and lasing. The model predicts fast depopulation of the ground 3s²3p state by the absorption of resonant laser light at 266 nm and very fast population of the excited 3s²4s state by the cascade transitions from the laser-pumped level, which is driven optically and by collisions. The SE of the 3s²3p-3s²4s transition at 396.15 nm is studied and possible SE at 1.3 and 2.1 μm is predicted. It is confirmed by calculations that the population inversion between the 3s²3p and 3s²4s states can be created by weak pumping at several microjoule–millijoule pulse energies and results in high gain. KW - Lasers KW - Spectroscopy KW - Atomic KW - Laser induced breakdown PY - 2017 DO - https://doi.org/10.1364/AO.56.000695 VL - 56 IS - 3 SP - 695 EP - 701 PB - Optical Society of America AN - OPUS4-39427 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Gornushkin, Igor B. A1 - Kazakov, Alexander Ya. T1 - Kinetic model of stimulated emission created by resonance pumping of aluminum laser-induced plasma JF - Journal of Applied Physics N2 - Stimulated emission observed experimentally in an aluminum laser induced plasma is modeled via a kinetic approach. The simulated emission at several cascade transitions is created by a pump laser guided through the plasma at several microseconds after its creation and tuned in resonance with the strong 3s²3p-3s²4s transition at 266 nm. A two-dimensional space-time collisional radiative plasma model explains the creation of the Population inversion and lasing at wavelengths of 2100 nm and 396.1 nm. The population inversion for lasing at 2100 nm is created by depopulation of the ground 3s²3p state and population of the 3s²5s state via the absorption of the resonant radiation at 266 nm. The population inversion for lasing at 396.1 nm occurs during the laser pulse via the decay of the population of the pumped 3s²5s state to the excited 3s²4s state via cascade transitions driven optically and by collisions. In particular, efficient are the mixing transitions between neighboring states separated by small gaps on the order of kT at Plasma temperatures of 5000–10 000 K. The model predicts that the population inversion and corresponding gain may reach high values even at very moderate pump energy of several lJ per pulse. The efficiency of lasing at 2100 nm and 396.1 nm is estimated to be ~3% and 0.05%, correspondingly with respect to the pump laser intensity. The gain for lasing at 396.1 nm can reach as high as ~40 cm⁻¹. The polarization effect that the pump radiation at 266 nm imposes on the stimulated emission at 396.1 nm is discussed. The calculated results are favorably compared to experimental data. KW - Laser induced plasma KW - LIBS KW - Plasma modeling KW - Plasma diagnostics KW - Lasers PY - 2017 DO - https://doi.org/10.1063/1.4984912 SN - 0021-8979 SN - 1089-7550 VL - 121 IS - 21 SP - 213303-1 EP - 213303-11 AN - OPUS4-40693 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - CONF A1 - Gornushkin, Igor B. A1 - Kazakov, Alexander Ya. A1 - Panne, Ulrich A1 - Huber, N. A1 - Pedarnig, J.D. A1 - Eschlböck-Fuchs, S. A1 - Rössler, R. T1 - Calibration-free Monte Carlo method for laser induced breakdown spectroscopy N2 - Calibration-free LIBS via Monte Carlo approach T2 - 8-14.10.2017 SciX, Reno, NV, USA CY - Reno, NV, USA DA - 7.10.2016 KW - Laser induced plasma KW - LIBS KW - Plasma modeling KW - Plasma diagnostics KW - Lasers PY - 2017 AN - OPUS4-42298 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER - TY - JOUR A1 - Gojani, Ardian A1 - Palásti, David J. A1 - Paul, Andrea A1 - Galbács, G. A1 - Gornushkin, Igor B. T1 - Analysis and classification of liquid samples by spatial heterodyne spectroscopy JF - Applied Spectroscopy N2 - Spatial heterodyne spectroscopy (SHS) is used for quantitative analysis and classification of liquid samples. SHS is a version of a Michelson interferometer with no moving parts and with diffraction gratings in place of mirrors. The instrument converts frequency-resolved information into spatially resolved one and records it in the form of interferograms. The back-extraction of spectral information is done by the Fast Fourier transform. A SHS instrument is constructed with the resolving power 5000 and spectral range 522 - 593 nm. Two original technical solutions are used as compared to previous SHS instruments: the use of a high frequency diode pumped solid state (DPSS) laser for excitation of Raman spectra and a microscope-based collection system. Raman spectra are excited at 532 nm at the repetition rate 80 kHz. Raman shifts between 330 cm-1 and 1600 cm-1 are measured. A new application of SHS is demonstrated: for the first time it is used for quantitative Raman analysis to determine concentrations of cyclohexane in isopropanol and glycerol in water. Two calibration strategies are employed: univariate based on the construction of a calibration plot and multivariate based on partial least square regression (PLSR). The detection limits for both cyclohexane in isopropanol and glycerol in water are at a 0.5 mass% level. In addition to the Raman-SHS chemical analysis, classification of industrial oils (biodiesel, poly(1-decene), gasoline, heavy oil IFO380, polybutenes, and lubricant) is performed using their Raman-fluorescence spectra and principal component analysis (PCA). The oils are easily discriminated as they show distinct non-overlapping patterns in the space of principal components. KW - Spectroscopy KW - Atomic KW - Laser induced breakdown KW - Lasers PY - 2019 DO - https://doi.org/10.1177/0003702819863847 SN - 1943-3530 VL - 73 IS - 12 SP - 1409 EP - 1419 PB - Sage AN - OPUS4-48599 LA - eng AD - Bundesanstalt fuer Materialforschung und -pruefung (BAM), Berlin, Germany ER -