4.6 Article

Townsend to glow discharge transition for a nanosecond pulse plasma in helium: space charge formation and resulting electric field dynamics

Journal

PLASMA SOURCES SCIENCE & TECHNOLOGY
Volume 30, Issue 5, Pages -

Publisher

IOP Publishing Ltd
DOI: 10.1088/1361-6595/abf320

Keywords

glow discharge; electric field; nanosecond pulsed discharge; sheath formation; Stark polarization spectroscopy; fluid modeling

Funding

  1. Department of Energy, office of Fusion Energy Science [DE-SC-0021376, AT4010100]
  2. U.S. Department of Energy's National Nuclear Security Administration [DE-NA0003525]
  3. [DE-SC-0016053]
  4. [DE-SC-0020232]

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Stark polarization spectroscopy was used to study the temporal evolution of the electric field distribution in the cathode region of a nanosecond pulsed discharge in helium. The discharge initially developed as a diffuse, cathode-directed ionization wave with a Townsend-like feature before transitioning to a glow-like structure, with filament formation observed near the high voltage electrode. The fluid model showed that enhanced ionization near the cathode caused space charge formation responsible for the increase in electric field.
Stark polarization spectroscopy is used to investigate the temporal evolution of the electric field distribution in the cathode region of a nanosecond pulsed discharge in helium at 120 Torr. The measurements are performed on the He I transition at 492.19 nm, during the early stages of the discharge formation. The experimental results are compared with the predictions of a 1D fluid model. Time-resolved ICCD images show that the discharge develops as a diffuse, cathode-directed ionization wave with a Townsend-like feature before transitioning into a glow-like structure. Near anode instabilities characterized by filament formation were observed near the high voltage electrode. Within 30 ns, a reduction of the sheath thickness to about 250 mu m is observed, coinciding with a gradual increase of the discharge current and proportional increase in electric field at the cathode. The cathode electric field corresponding to this sheath with a thickness of 250 mu m is about 40 kV cm(-1). A subsequent steep increase of the discharge current leads to a further reduction of the sheath width. The electric field evolution as obtained by the fluid model is in excellent agreement with the measurements and shows that an enhanced ionization near the cathode is causing the space charge formation responsible for the increase in electric field.

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