Neutral depletion and the helicon density limit
Author(s) -
Richard Magee,
Matthew Galante,
Jerry Carr,
Greg Lusk,
Dustin McCarren,
Earl Scime
Publication year - 2013
Publication title -
physics of plasmas
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.75
H-Index - 160
eISSN - 1089-7674
pISSN - 1070-664X
DOI - 10.1063/1.4849376
Subject(s) - helicon , physics , atomic physics , plasma , ionization , electron density , electron temperature , electron , krypton , energetic neutral atom , antenna (radio) , limit (mathematics) , ion , argon , nuclear physics , electrical engineering , quantum mechanics , engineering , mathematical analysis , mathematics
It is straightforward to create fully ionized plasmas with modest rf power in a helicon. It is difficult, however, to create plasmas with density >1020 m−3, because neutral depletion leads to a lack of fuel. In order to address this density limit, we present fast (1 MHz), time-resolved measurements of the neutral density at and downstream from the rf antenna in krypton helicon plasmas. At the start of the discharge, the neutral density underneath the antenna is reduced to 1% of its initial value in 15 μs. The ionization rate inferred from these data implies that the electron temperature near the antenna is much higher than the electron temperature measured downstream. Neutral density measurements made downstream from the antenna show much slower depletion, requiring 14 ms to decrease by a factor of 1/e. Furthermore, the downstream depletion appears to be due to neutral pumping rather than ionization.
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