2020
DOI: 10.1109/tps.2020.3026734
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A New Computer Simulation of Avalanche Evolution and Its Transition Into Anode- and Cathode-Directed Streamers in Short Uniform Field Gaps

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Cited by 4 publications
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“…where γ ph is Townsend's second ionization coefficient due to the action of photons at the cathode, μ is the photon absorption coefficient [10] in the gas, g(z) is a geometry factor to account for the photons received at the cathode from the primary avalanche during its growth at distance z along the gap axis and d is the gap spacing [9].…”
Section: Fig 1 Growth Of Avalanche In Uniform-field Gapmentioning
confidence: 99%
“…where γ ph is Townsend's second ionization coefficient due to the action of photons at the cathode, μ is the photon absorption coefficient [10] in the gas, g(z) is a geometry factor to account for the photons received at the cathode from the primary avalanche during its growth at distance z along the gap axis and d is the gap spacing [9].…”
Section: Fig 1 Growth Of Avalanche In Uniform-field Gapmentioning
confidence: 99%