Laser interaction with undercritical foams of different spatial structures
The interaction of high-power laser pulses with undercritical foams produced by different techniques but with the same average density is studied at the PALS laser facility. The spatial–temporal evolution of X-ray emission is observed using an X-ray streak camera, electron and ion temperatures are m...
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AIP Publishing LLC
2025-01-01
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Series: | Matter and Radiation at Extremes |
Online Access: | http://dx.doi.org/10.1063/5.0225997 |
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author | J. Limpouch V. Tikhonchuk O. Renner Sh. Agarwal T. Burian J. Červenka J. Dostál R. Dudžák D. Ettel A. Gintrand L. Hudec L. Juha O. Klimo M. Krupka M. Krus T. Lastovicka R. Liska W. Nazarov S. K. Singh M. Šilhavík S. Weber |
author_facet | J. Limpouch V. Tikhonchuk O. Renner Sh. Agarwal T. Burian J. Červenka J. Dostál R. Dudžák D. Ettel A. Gintrand L. Hudec L. Juha O. Klimo M. Krupka M. Krus T. Lastovicka R. Liska W. Nazarov S. K. Singh M. Šilhavík S. Weber |
author_sort | J. Limpouch |
collection | DOAJ |
description | The interaction of high-power laser pulses with undercritical foams produced by different techniques but with the same average density is studied at the PALS laser facility. The spatial–temporal evolution of X-ray emission is observed using an X-ray streak camera, electron and ion temperatures are measured by X-ray spectroscopy, and hot-electron production is characterized by monochromatic X-ray imaging. Transmission of a femtosecond laser probe pulse through foams is observed in the near and far fields. In spite of large differences in pore size and foam structure, the velocity of ionization front propagation is quite similar for all the foams studied and is slower than that in a homogeneous material of the same average density. The ion temperature in the plasma behind the ionization front is a few times higher than the electron temperature. Hot-electron production in plastic foams with small pores is strongly suppressed compared with that in solid targets, whereas in foams produced by additive manufacturing, it is significantly increased to the level observed in bare copper foil targets. |
format | Article |
id | doaj-art-3dbf5c1fd77a4458be983bedce124bb8 |
institution | Kabale University |
issn | 2468-080X |
language | English |
publishDate | 2025-01-01 |
publisher | AIP Publishing LLC |
record_format | Article |
series | Matter and Radiation at Extremes |
spelling | doaj-art-3dbf5c1fd77a4458be983bedce124bb82025-02-03T16:33:24ZengAIP Publishing LLCMatter and Radiation at Extremes2468-080X2025-01-01101017402017402-910.1063/5.0225997Laser interaction with undercritical foams of different spatial structuresJ. Limpouch0V. Tikhonchuk1O. Renner2Sh. Agarwal3T. Burian4J. Červenka5J. Dostál6R. Dudžák7D. Ettel8A. Gintrand9L. Hudec10L. Juha11O. Klimo12M. Krupka13M. Krus14T. Lastovicka15R. Liska16W. Nazarov17S. K. Singh18M. Šilhavík19S. Weber20Faculty of Nuclear Science and Physical Engineering, Czech Technical University in Prague, 115 19 Prague, Czech RepublicThe Extreme Light Infrastructure ERIC, ELI-Beamlines Facility, Za Radnicí 835, 252 41 Dolní Břežany, Czech RepublicThe Extreme Light Infrastructure ERIC, ELI-Beamlines Facility, Za Radnicí 835, 252 41 Dolní Břežany, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicThe Extreme Light Infrastructure ERIC, ELI-Beamlines Facility, Za Radnicí 835, 252 41 Dolní Břežany, Czech RepublicFaculty of Nuclear Science and Physical Engineering, Czech Technical University in Prague, 115 19 Prague, Czech RepublicInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicFaculty of Nuclear Science and Physical Engineering, Czech Technical University in Prague, 115 19 Prague, Czech RepublicFaculty of Nuclear Science and Physical Engineering, Czech Technical University in Prague, 115 19 Prague, Czech RepublicInstitute of Plasma Physics, Czech Academy of Sciences, 182 00 Prague, Czech RepublicThe Extreme Light Infrastructure ERIC, ELI-Beamlines Facility, Za Radnicí 835, 252 41 Dolní Břežany, Czech RepublicFaculty of Nuclear Science and Physical Engineering, Czech Technical University in Prague, 115 19 Prague, Czech RepublicIndependent Foam Target Supplier, St. Andrews, Fife, ScotlandInstitute of Physics, Czech Academy of Sciences, Na Slovance 1999/2, 182 00 Prague, Czech RepublicFaculty of Nuclear Science and Physical Engineering, Czech Technical University in Prague, 115 19 Prague, Czech RepublicThe Extreme Light Infrastructure ERIC, ELI-Beamlines Facility, Za Radnicí 835, 252 41 Dolní Břežany, Czech RepublicThe interaction of high-power laser pulses with undercritical foams produced by different techniques but with the same average density is studied at the PALS laser facility. The spatial–temporal evolution of X-ray emission is observed using an X-ray streak camera, electron and ion temperatures are measured by X-ray spectroscopy, and hot-electron production is characterized by monochromatic X-ray imaging. Transmission of a femtosecond laser probe pulse through foams is observed in the near and far fields. In spite of large differences in pore size and foam structure, the velocity of ionization front propagation is quite similar for all the foams studied and is slower than that in a homogeneous material of the same average density. The ion temperature in the plasma behind the ionization front is a few times higher than the electron temperature. Hot-electron production in plastic foams with small pores is strongly suppressed compared with that in solid targets, whereas in foams produced by additive manufacturing, it is significantly increased to the level observed in bare copper foil targets.http://dx.doi.org/10.1063/5.0225997 |
spellingShingle | J. Limpouch V. Tikhonchuk O. Renner Sh. Agarwal T. Burian J. Červenka J. Dostál R. Dudžák D. Ettel A. Gintrand L. Hudec L. Juha O. Klimo M. Krupka M. Krus T. Lastovicka R. Liska W. Nazarov S. K. Singh M. Šilhavík S. Weber Laser interaction with undercritical foams of different spatial structures Matter and Radiation at Extremes |
title | Laser interaction with undercritical foams of different spatial structures |
title_full | Laser interaction with undercritical foams of different spatial structures |
title_fullStr | Laser interaction with undercritical foams of different spatial structures |
title_full_unstemmed | Laser interaction with undercritical foams of different spatial structures |
title_short | Laser interaction with undercritical foams of different spatial structures |
title_sort | laser interaction with undercritical foams of different spatial structures |
url | http://dx.doi.org/10.1063/5.0225997 |
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