Author Affiliations
Abstract
1 Department of Radiation and Chemical Physics, Institute of Physics, Czech Academy of Sciences, Na Slovance 2, 182 21 Prague 8, Czech Republic
2 Laser Plasma Department, Institute of Plasma Physics, Czech Academy of Sciences, Za Slovankou 3, 182 00 Prague 8, Czech Republic
3 Department of Surface and Plasma Science, Faculty of Mathematics and Physics, Charles University in Prague, V Holešovičkách 2, 180 00 Prague 8, Czech Republic
4 Department of Physical Electronics, Faculty of Nuclear Science and Engineering Physics, Czech Technical University in Prague, V Holešovičkách 2, 180 00 Prague 8, Czech Republic
5 Helmholtz-Zentrum Dresden-Rossendorf, Bautzner Landstraße 400, 01328 Dresden, Germany
6 DESY Photon Science, Notkestraße 85, D-22607 Hamburg, Germany
7 Institut de Minéralogie, de Physique des Matériaux et de Cosmochimie, UMR 7590 – UPMC/CNRS/IRD/MNHN, Sorbonne Université, 4 place Jussieu, 75005 Paris, France
8 Department of Physics, Faculty of Electrical Engineering, Czech Technical University in Prague, Technická 2, 166 27 Prague 6, Czech Republic
9 Center for Soft Nanoscience, University of Münster, Busso-Peus-Straße 10, D-48149 Münster, Germany
We report on an experiment performed at the FLASH2 free-electron laser (FEL) aimed at producing warm dense matter via soft x-ray isochoric heating. In the experiment, we focus on study of the ions emitted during the soft x-ray ablation process using time-of-flight electron multipliers and a shifted Maxwell–Boltzmann velocity distribution model. We find that most emitted ions are thermal, but that some impurities chemisorbed on the target surface, such as protons, are accelerated by the electrostatic field created in the plasma by escaped electrons. The morphology of the complex crater structure indicates the presence of several ion groups with varying temperatures. We find that the ion sound velocity is controlled by the ion temperature and show how the ion yield depends on the FEL radiation attenuation length in different materials.
Matter and Radiation at Extremes
2024, 9(1): 016602
Author Affiliations
Abstract
1 HiLASE Centre, Institute of Physics ASCR, v.v.i., Za Radnici 825, 25241 Dolni Brezany, Czech Republic
2 Czech Technical University, Thakurova 2077/7, 160 00 Prague 6, Czech Republic
3 Laser Laboratorium Gottingen (LLG), 37077 Gottingen, Germany
4 Department of Electrical and Computer Engineering, Colorado State University, Fort Collins, CO 80523, USA
A preliminary investigation on short-wavelength ablation mechanisms of poly(methyl methacrylate) (PMMA) and poly (1,4-phenylene ether ether-sulfone) (PPEES) by extreme ultraviolet (EUV) radiation at 13.5 nm using a table-top laserproduced plasma from a gas-puff target at LLG (Gottingen) and at 46.9 nm by a 10 Hz desktop capillary discharge laser operated at the Institute of Physics (Prague) is presented. Ablation of polymer materials is initiated by photoinduced polymer chain scissions. The ablation occurs due to the formation of volatile products by the EUV radiolysis removed as an ablation plume from the irradiated material into the vacuum. In general, cross-linking of polymer molecules can compete with the chain decomposition. Both processes may influence the efficiency and quality of micro(nano)structuring in polymer materials. Wavelength is a critical parameter to be taken into account when an EUV ablation process occurs, because different wavelengths result in different energy densities in the near-surface region of the polymer exposed to nanosecond pulses of intense EUV radiation.
EUV ablation organic polymer photo-erosion mechanisms wavelength effect 
High Power Laser Science and Engineering
2014, 2(3): 03000e26

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