Quantum Beam Science (Jan 2024)
A Platform for Laser-Driven Ion Sources Generated with Nanosecond Laser Pulses in the Intensity Range of 10<sup>13</sup>–10<sup>15</sup> W/cm<sup>2</sup>
- L. Giuffrida,
- V. Istokskaia,
- A. Picciotto,
- V. Kantarelou,
- M. Barozzi,
- R. Dell`Anna,
- M. Divoky,
- O. Denk,
- D. Giubertoni,
- F. Grepl,
- A. Hadjikyriacou,
- M. Hanus,
- J. Krasa,
- M. Kucharik,
- T. Levato,
- P. Navratil,
- J. Pilar,
- F. Schillaci,
- S. Stancek,
- M. Tosca,
- M. Tryus,
- A. Velyhan,
- A. Lucianetti,
- T. Mocek,
- D. Margarone
Affiliations
- L. Giuffrida
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- V. Istokskaia
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- A. Picciotto
- Micro-Nano Facility, Sensors and Devices, Fondazione Bruno Kessler, 38121 Trento, Italy
- V. Kantarelou
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- M. Barozzi
- Micro-Nano Facility, Sensors and Devices, Fondazione Bruno Kessler, 38121 Trento, Italy
- R. Dell`Anna
- Micro-Nano Facility, Sensors and Devices, Fondazione Bruno Kessler, 38121 Trento, Italy
- M. Divoky
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- O. Denk
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- D. Giubertoni
- Micro-Nano Facility, Sensors and Devices, Fondazione Bruno Kessler, 38121 Trento, Italy
- F. Grepl
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- A. Hadjikyriacou
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- M. Hanus
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- J. Krasa
- Institute of Physics ASCR, v.v.i (FZU), 10000 Prague, Czech Republic
- M. Kucharik
- Faculty of Nuclear Sciences and Physical Engineering, Czech Technical University in Prague, 11519 Prague, Czech Republic
- T. Levato
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- P. Navratil
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- J. Pilar
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- F. Schillaci
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- S. Stancek
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- M. Tosca
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- M. Tryus
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- A. Velyhan
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- A. Lucianetti
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- T. Mocek
- HiLASE Centre, Institute of Physics of the Czech Academy of Sciences, 25241 Dolni Brezany, Czech Republic
- D. Margarone
- ELI Beamlines Facility, The Extreme Light Infrastructure ERIC, 25241 Dolni Brezany, Czech Republic
- DOI
- https://doi.org/10.3390/qubs8010005
- Journal volume & issue
-
Vol. 8,
no. 1
p. 5
Abstract
An experimental platform for laser-driven ion (sub-MeV) acceleration and potential applications was commissioned at the HiLASE laser facility. The auxiliary beam of the Bivoj laser system operating at a GW level peak power (~10 J in 5–10 ns) and 1–10 Hz repetition rate enabled a stable production of high-current ion beams of multiple species (Al, Ti, Fe, Si, Cu, and Sn). The produced laser–plasma ion sources were fully characterized against the laser intensity on the target (1013–1015 W/cm2) by varying the laser energy, focal spot size, and pulse duration. The versatility and tuneability of such high-repetition-rate laser–plasma ion sources are of potential interest for user applications. Such a statistically accurate study was facilitated by the large amount of data acquired at the high repetition rate (1–10 Hz) provided by the Bivoj laser system.
Keywords