Studies of gas ionization by high-power, sub-nanosecond microwave pulses

This study investigates the ionization pressure threshold of a gas (air, helium, argon, and SF6 across a wide pressure range) filled dielectric tube when a ∼300 MW, ∼0.7 ns, 9.6 GHz high-power microwave (HPM) pulse propagates through it. The thresholds are determined as the pressure for which the energy of the transmitted HPM pulse decreases to ∼30%, which is close to the same HPM pulse's transmission coefficient when a metal rod fills the tube. These thresholds are found to be 0.4 × 105 Pa,105 Pa, 1.8 × 105 Pa, and 0.2 × 105 Pa, for air, argon, helium, and SF6, respectively. The measured intensity of the plasma light emission starts to decrease at a pressure which coincides with the pressure threshold determined by HPM pulse propagation. Additionally, at gas pressures <5 × 104 Pa, it is shown that time- and space-resolved images of the light emission display a diffused plasma which at higher pressures >105 Pa transforms into streamer like plasma. Simplified numerical simulations of a microwave discharge in air at 1 × 105 Pa and 4 × 105 Pa are consistent with the experimental plasma light observations.

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Publication Details

Journal
Physics of Plasmas
Published
2024-12-01
DOI
https://doi.org/10.1063/5.0238887
Citations
5
Primary Topic
Gyrotron and Vacuum Electronics Research
Type
article
Field-Weighted Citation Impact
1.69

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article

Studies of gas ionization by high-power, sub-nanosecond microwave pulses

J. G. Leopold, V. Maksimov, Yang Cao, Ya. E. Krasik et al.
5 citations
Physics of Plasmas
Gyrotron and Vacuum Electronics Research
1.69
article

Studies of gas ionization by high-power, sub-nanosecond microwave pulses

J. G. Leopold, V. Maksimov, Yang Cao, Ya. E. Krasik, Alexander Yu. Kostinskiy, Nikita Asmedianov, A. Haim
article en
5 citations

Abstract

This study investigates the ionization pressure threshold of a gas (air, helium, argon, and SF6 across a wide pressure range) filled dielectric tube when a ∼300 MW, ∼0.7 ns, 9.6 GHz high-power microwave (HPM) pulse propagates through it. The thresholds are determined as the pressure for which the energy of the transmitted HPM pulse decreases to ∼30%, which is close to the same HPM pulse's transmission coefficient when a metal rod fills the tube. These thresholds are found to be 0.4 × 105 Pa,105 Pa, 1.8 × 105 Pa, and 0.2 × 105 Pa, for air, argon, helium, and SF6, respectively. The measured intensity of the plasma light emission starts to decrease at a pressure which coincides with the pressure threshold determined by HPM pulse propagation. Additionally, at gas pressures <5 × 104 Pa, it is shown that time- and space-resolved images of the light emission display a diffused plasma which at higher pressures >105 Pa transforms into streamer like plasma. Simplified numerical simulations of a microwave discharge in air at 1 × 105 Pa and 4 × 105 Pa are consistent with the experimental plasma light observations.

Physics of PlasmasVol. 31(12)
Technion – Israel Institute of Technology (IL)
PAZY Foundation
Affordable and clean energy
Openalex Percentile: Top 15%
Gyrotron and Vacuum Electronics Research
1.69
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