Bulletin of the American Physical Society
74th Annual Gaseous Electronics Conference
Volume 66, Number 7
Monday–Friday, October 4–8, 2021;
Virtual: GEC Platform
Time Zone: Central Daylight Time, USA
Session PR23: AMP Gateway and Electron Collisions
10:15 AM–12:30 PM,
Thursday, October 7, 2021
Room: GEC platform
Chair: Robin Cote, University of Massachusetts Boston
Abstract: PR23.00006 : Absolute O atom density measurements by actinometry: comparison to cavity ring-down spectroscopy
12:00 PM–12:15 PM
Presenter:
Edmond Baratte
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, Ecole Polytechnique Institut Polytechnique de Paris, 91128 Palaiseau France)
Authors:
Edmond Baratte
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, Ecole Polytechnique Institut Polytechnique de Paris, 91128 Palaiseau France)
Andrey Volynets
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, Ecole Polytechnique Institut Polytechnique de Paris, 91128 Palaiseau France)
Dmitry Lopaev
(Moscow State University, Skobeltsyn Institute of Nuclear Physics, Microelectronics Dep., Moscow, Russia)
Cherif Si Moussi
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, Ecole Polytechnique Institut Polytechnique de Paris, 91128 Palaiseau France)
Jean-Paul Booth
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, Ecole Polytechnique Institut Polytechnique de Paris, 91128 Palaiseau France)
Olivier Guaitella
(Laboratoire de Physique des Plasmas (LPP), CNRS, Sorbonne Université, Ecole Polytechnique Institut Polytechnique de Paris, 91128 Palaiseau France)
We have evaluated the validity of O actinometry by comparison to cavity ring-down (CRDS) measurements. We measured both in continuous glow discharges in various mixtures of oxygen, CO2, Ar and Kr at pressures between 1 and 5 Torr.
The emission is monitored with an Isoplane SCT320 spectrometer and with an OceanOptics Maya USB spectrometer. The O atom density is determined by CRDS using the O(1D2)↔O(3PJ) transition at 15,867.8cm-1.
The electric field in the tube is measured directly, allowing computation of the EEDF with the LoKI Boltzmann solver. The O atom density was then calculated from the excitation cross-sections and the line intensities.
Large discrepancies are found between CRDS and actinometry using the IST-Lisbon oxygen dataset for the EEDF and common cross-sections for the lines of interest. We also propose a method to estimate the reduced electric field from the ratio of atomic emission lines.
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