2015
DOI: 10.1103/physreve.91.043106
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Physics of giant electromagnetic pulse generation in short-pulse laser experiments

Abstract: In this paper we describe the physical processes that lead to the generation of giant electromagnetic pulses (GEMPs) at powerful laser facilities. Our study is based on experimental measurements of both the charging of a solid target irradiated by an ultra-short, ultra-intense laser and the detection of the electromagnetic emission in the GHz domain. An unambiguous correlation between the neutralization current in the target holder and the electromagnetic emission shows that the source of the GEMP is the remai… Show more

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Cited by 114 publications
(123 citation statements)
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“…The primary mechanism responsible for generating such high electromagnetic fields in a laser-plasma interaction is typically attributed to ejection of a large flux of energetic ‘hot’ electrons from the plasma followed by a transient ‘slow’ electron return current through the target mount to re-establish quasi-neutrality in the plasma 10, 11, 13, 21 . EMP can be extremely problematic in high-power laser experiments, as EMP signals lasting for hundreds of nanoseconds often adversely affect nearby electronic systems, possibly resulting in loss of data or even permanent damage to high-value equipment.…”
Section: Introductionmentioning
confidence: 99%
“…The primary mechanism responsible for generating such high electromagnetic fields in a laser-plasma interaction is typically attributed to ejection of a large flux of energetic ‘hot’ electrons from the plasma followed by a transient ‘slow’ electron return current through the target mount to re-establish quasi-neutrality in the plasma 10, 11, 13, 21 . EMP can be extremely problematic in high-power laser experiments, as EMP signals lasting for hundreds of nanoseconds often adversely affect nearby electronic systems, possibly resulting in loss of data or even permanent damage to high-value equipment.…”
Section: Introductionmentioning
confidence: 99%
“…The ultra-short EM pulses with peak electric field of the order of 10 9 V m −1 , are generated following the rapid charging of the laser-irradiated target to MV potential, due to the prompt escape of the high energy (MeV) electrons produced during the interaction [2,13,19] . The EM pulse was observed propagating along a thin metallic wire attached to the main foil target.…”
Section: Introductionmentioning
confidence: 99%
“…The majority of them spread out and dissipate energy, while only the fastest component can reach the target rear side [31]. Afterwards, the most energetic electrons escape, leaving an electrostatic potential on target, due to the unbalanced positive charge left on it [32]. Such potential generates an electric field that ionizes and accelerates surface ions in a process called Target Normal Sheath Acceleration (TNSA) [29].…”
Section: Eos Diagnostics For Fs Resolution Probing High Intensity Lasmentioning
confidence: 99%