29 June 2026 to 3 July 2026
EICC, Edinburgh
Europe/London timezone

Broadband Electromagnetic Pulse Emission at the Sub-Nanosecond Kilojoule Laser PALS

Not scheduled
20m
EICC, Edinburgh

EICC, Edinburgh

150 Morrison St, Edinburgh EH3 8EE
Poster Presentation Laser and Particle Beam Interaction with Plasmas, Hydrodynamics and Instabilities (BPIF)

Description

Interaction of high-power lasers with matter is accompanied by intense electromagnetic pulses (EMP), which can interfere with diagnostics and damage sensitive electronics, requiring mitigation. At the same time, intense EMPs offer potential for advanced applications. In fundamental plasma physics, laser-driven EMP remains of intrinsic interest, as its generation mechanisms are not yet fully understood.
At the PALS laser facility (1315 nm, 200–300 ps, up to 700 J on target), EMP has been systematically studied for solid, foam, and gaseous targets in both near- and far-field regions. Using a comprehensive broadband diagnostic setup (B-dot and D-dot probes, antennas, target current and voltage probes, low-loss cables, and oscilloscopes with 100 GS/s sampling rate and 33 GHz bandwidth), we observed an exceptionally broad EMP spectrum extending up to 20 GHz. Both peak and centroid frequencies strongly depend on laser intensity, determined by pulse energy and focal spot size, for both polarizations.
At maximum intensities (~2 × 10¹⁷ W/cm²), the neutralization current reached 10 kA. Far-field antenna measurements indicate a total emitted multi-GHz EMP power on the order of GW, corresponding to ~0.1% of the laser pulse energy. The electric field strength at 1 m from the target reached approximately 1 MV/m.
The observed spectral dependence on laser intensity suggests that EMP generation is closely related to plasma dynamics and electron oscillations, whose energy distributions are strongly intensity-dependent.

This research is supported by the Grant Agency of the Czech Republic (Grant No. GM23 05027M), Czech Republic’s Ministry of Education, Youth and Sports project Prague Asterix Laser System (LM2023068) and the EUROfusion Consortium - Euroatom Research and Training Program (Grant No.101052200-EUROfusion). The involved teams have operated within the framework of the Enabling Research Project AWP24-ENR-IFE.02.CEA-01 “Magnetized ICF”.

[1] J. Cikhardt, P. W. Bradford, M. Ehret, S. Agarwal, M. Alonzo, et al:
Comprehensive characterization of electromagnetic pulses driven by a sub-nanosecond kilojoule laser, High Power Laser Science and Engineering 13, e57 (2025)

[2] V. Horká-Zelenková, J. Krása, M. Toufarová, J. Cikhardt, P. Devi, et al: “Electromagnetic pulses, optical emission and chemical change associated with high-power laser-induced dielectric breakdown of gaseous sulphur hexafluoride”, High Power Laser Science and Engineering 13, e77 (2025)

[3] P Rączka, J. Cikhardt, M. Pfeifer, J. Krása, M. Krupka, et al:
“Measurement of strong electromagnetic pulses generated from solid targets at sub-ns kJ-class PALS laser facility”,Plasma Phys. Control. Fusion 63, 085015 (2021)

[4] J. Cikhardt, J. Krása, S. Agarwal, M. Alonzo, P.W. Bradford,
M.Červeňák, et al: “Study of electromagnetic pulses with frequencies exceeding 10 GHz at the kilojoule sub-nanosecond laser facility PALS”, submitted to Plasma Phys. Control. Fusion in November 2025

Author

Jakub Cikhardt (Czech technical university in Prague)

Co-authors

Dr A. Da Ros (University of Bordeaux) Prof. A. Morace (Institute of Physics CAS) Dr B. Cikhardtova (Czech Technical University in Prague) Mr B. Grau (Universita di Roma Tor Vergata) Claudio Verona (Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tor Vergata, Roma, Italy and Università di Roma “Tor Vergata”, Dipartimento di Ingegneria Industriale, Roma, Italy) Prof. D. Klir (Czech Technical University in Prague) Fabrizio Consoli (Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tor Vergata, Via della Ricerca Scientifica, Roma, Italy and ENEA - Dipartimento Fusione e Tecnologie per la Sicurezza Nucleare, Frascati, Italy) Mr J. Loffelmann (Czech Technical University in Prague) Mr J. Malir (Czech Technical University in Prague) Mr J. Novotny (Czech Technical University in Prague) Jan Proska (Faculty of Nuclear Science and Physical Engineering, Czech Technical University, Prague, Czech Republic) Josef Krása (Institute of Physics of the Czech Academy of Sciences) João Jorge Santos (CELIA, Université de Bordeaux, CNRS, UMR 5107, 33405 Talence, France) Libor Juha (Institute of Physics, Czech Academy of Sciences, Prague, Czech Republic) Dr M. Alonzo (ENEA Frascati) Mr M. Cervenak (Institute of Plasma Physics CAS) Dr M. Ehret (ERIC ELI Beamlines Czech Republic) Dr M. Toufarova (Institute of Physics CAS) Massimiliano Scisciò (Istituto Nazionale di Fisica Nucleare, Sezione di Roma Tor Vergata, Roma, Italy and ENEA - Dipartimento Fusione e Tecnologie per la Sicurezza Nucleare, CR Frascati, Frascati, Italy) Michal Krupka (Institute of Plasma Physics, Czech Academy of Sciences, Prague, Czech Republic) Dr O. Renner (Institute of Physics CAS) Mr O. Zajan (Czech Technical University in Prague) Ondrej Klimo (Faculty of Nuclear Science and Physical Engineering, Czech Technical University, Prague, Czech Republic) Mr P. Gajdos (Institute of Plasma Physics CAS) Dr P.W. Bradford (CLF RAL, Chilton UK) Pooja Devi (Charles University, FZU-Czech Acadermia of Sciences) Roman Dudzak (Institute of Physics, Czech Academy of Sciences, Prague, Czech Republic) Shubham Agarwal (Institute of Physics, Czech Academy of Sciences, Prague, Czech Republic) Simon Jelinek (Institute of Plasma Physics, Czech Academy of Sciences, Prague, Czech Republic) Sushil Singh (Institute of Physics of the Czech Academy of Sciences) Dr V. Horka-Zelenkova (Institute of Physics CAS) Dr V. Munzar (Czech Technical University in Prague)

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