77th Annual Gaseous Electronics Conference
Monday–Friday, September 30–October 4 2024;
San Diego, California
Session HT4: Poster Session I (4:00pm-6:00pm)
4:00 PM,
Tuesday, October 1, 2024
Room: Gallery & Great Room 1-4
Abstract: HT4.00047 : The spatial profile of argon metastable species in an electron beam generated plasma*
Abstract
Presenter:
V S Santosh K Kondeti
(Princeton Plasma Physics Laboratory)
Authors:
V S Santosh K Kondeti
(Princeton Plasma Physics Laboratory)
Nirbhav S Chopra
(Princeton Plasma Physics Laboratory)
Shurik Yatom
(Princeton Plasma Physics Laboratory)
Yevgeny Raitses
(Princeton Plasma Physics Laboratory)
Electron beam (e-beam) generated plasmas offer a method to tailor the material processing outcomes by controlling the electron energy while maintaining a low electron temperature[i]. They facilitate the generation of low-energy ions at the periphery of the primary electron beam due to the presence of metastable species in the periphery of the discharge[ii] and produce plasma-chemistry[iii]. In this work, we measured the absolute density of argon (1s
5) metastables in an e-beam generated ExB secondary electron emission plasma source using laser-induced fluorescence. The electron temperature and the electron density were determined using a Langmuir probe. Both the electron and the Ar (1s
5) densities were found to be of the order of 10
16 m
-3, while the electron temperature was found to be below an energy of 1eV. Both the electron and the Ar (1s
5) densities decreased with the radial distance from the center of the discharge, while the electron temperature remained constant. The Ar (1s
5) density was found to have two regions of density decay, one within the active e-beam region and the other outside the e-beam. The region outside the e-beam can be explained by an Ar (1s
5) diffusion profile, while the e-beam region has a production term coupled with diffusion. The discharge current increases with pressure due to the enhancement of the collision frequency. This results in the observed increase in the e-beam diameter and the electron density with pressure. The size of the e-beam as a function of pressure was demarked by the start of the diffusion only region at a larger radial distance from the center of the discharge. The electron temperature of the secondary electrons as a function of pressure also increased, consistent with the previous observations
i. The Ar (1s
5) density, both in the e-beam and outside the e-beam regions increase as a function of pressure, suggesting the production of more metastables with the increase in pressure.
[i] Lock E, Fernsler R and Walton S, Plasma Sources Science and Technology, 17 025009 (2008).
[ii] S. G. Walton et al., ECS Journal of Solid State Science and Technology, 4(6) N5033 (2015).
[iii] S. Yatom et al., Plasma Sources Science and Technology, 32 115005 (2023).
*This work was supported by the U.S. Department of Energy through contract DE-AC02-09CH11466.