Microwave breakdown of sub-atmospheric argon gas in the vicinity of a microgap

The microwave electric field at breakdown for argon gas in a microgap (generally, gap size <1 mm) over a wide range of pressures and gap sizes was found to exhibit two behavioral pressure regimes. A high microwave electric field was established in the gap of a re-entrant mode resonator. By slowly...

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Bibliographic Details
Main Authors: Hernandez, M.E.C (Author), Kellner, Z.T (Author), Lenters, G.T (Author), Medema, A.R (Author), Remillard, S.K (Author), Woodwyk, S.M (Author), Zywicki, W.G (Author)
Format: Article
Language:English
Published: American Institute of Physics Inc. 2022
Subjects:
Online Access:View Fulltext in Publisher
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020 |a 21583226 (ISSN) 
245 1 0 |a Microwave breakdown of sub-atmospheric argon gas in the vicinity of a microgap 
260 0 |b American Institute of Physics Inc.  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1063/5.0082854 
520 3 |a The microwave electric field at breakdown for argon gas in a microgap (generally, gap size <1 mm) over a wide range of pressures and gap sizes was found to exhibit two behavioral pressure regimes. A high microwave electric field was established in the gap of a re-entrant mode resonator. By slowly raising the microwave electric field level, a breakdown level is reached where impact ionization induces low pressure argon gas to breakdown preferentially outside of the gap. At high pressure, breakdown is found to occur preferentially inside the gap, but only after the pressure is high enough for impact ionization to produce breakdown there. Impact ionization has a lower threshold electric field than the boundary-controlled processes, such as secondary electron emission, that would eventually produce breakdown inside the microgap if impact ionization did not occur first. Thus, the lower pressure regime is characterized by breakdown outside of the gap, while in the high-pressure regime, breakdown occurs inside the gap, in both cases by impact ionization. The transition pressure PT between these two pressure regimes depends on the gap size dgap, roughly as PT ∝ dgap-2. Consistent with the model developed here, this corresponds to the full-amplitude of electron oscillation in the gap field being commensurate with the gap size. © 2022 Author(s). 
650 0 4 |a Argon 
650 0 4 |a Argon gas 
650 0 4 |a Atmospheric argon 
650 0 4 |a Electric fields 
650 0 4 |a Gap size 
650 0 4 |a High microwave 
650 0 4 |a High pressure 
650 0 4 |a Impact ionization 
650 0 4 |a Ionization of gases 
650 0 4 |a Low pressures 
650 0 4 |a Micro gaps 
650 0 4 |a Microwave breakdown 
650 0 4 |a Microwave electric field 
650 0 4 |a Microwave resonators 
650 0 4 |a Microwaves 
650 0 4 |a Pressure regime 
650 0 4 |a Secondary emission 
700 1 |a Hernandez, M.E.C.  |e author 
700 1 |a Kellner, Z.T.  |e author 
700 1 |a Lenters, G.T.  |e author 
700 1 |a Medema, A.R.  |e author 
700 1 |a Remillard, S.K.  |e author 
700 1 |a Woodwyk, S.M.  |e author 
700 1 |a Zywicki, W.G.  |e author 
773 |t AIP Advances