EFFECTS OF WALL RECOMBINATION ON THE ETCH RATE AND PLASMA COMPOSITIONOF AN ETCH REACTOR

Citation
Gi. Font et al., EFFECTS OF WALL RECOMBINATION ON THE ETCH RATE AND PLASMA COMPOSITIONOF AN ETCH REACTOR, Journal of vacuum science & technology. A. Vacuum, surfaces, and films, 16(4), 1998, pp. 2057-2064
Citations number
10
Categorie Soggetti
Physics, Applied","Materials Science, Coatings & Films
ISSN journal
07342101
Volume
16
Issue
4
Year of publication
1998
Pages
2057 - 2064
Database
ISI
SICI code
0734-2101(1998)16:4<2057:EOWROT>2.0.ZU;2-Q
Abstract
A helicon plasma etch reactor is simulated using direct simulation Mon te Carlo and particle-in-cell methods for a chlorine (Cl-2) feed gas f low. Computations for the gas discharge are carried out by modeling th e ions and neutrals as particles and by imposing the electrons as a ba ckground condition conforming to experimental measurements. The neutra ls and ions are then allowed to interact with the background electrons and to relax to a steady state. The effects on the reactor flow field and etch rate of chlorine atom recombination into chlorine molecules at the walls is investigated. Results show that recombination at the w alls results in the depletion of the amount of chlorine atoms (Cl) in the reactor. The depleted chlorine atom population leads to lower ioni zation levels and a diminished ion (Cl+) flux to the wafer. Consequent ly, the etch rate is decreased by as much as 15% when compared to simu lations without recombination. The creation of chlorine (Cl-2) molecul es at the walls through recombination also provides a new source for n egative ions (Cl-) which increases the electronegativity of the plasma . In addition, the results of the simulation are compared with ion cur rent and optical emission spectroscopy (OES) measurements. The Cl-Ar r atio (measured by the OES technique) increases less than 20% from the centerline to the wall of the reactor. An inspection of absolute densi ties, however, reveals that the individual near-wall densities are as much as a factor of 2 greater than the centerline densities. The trace species, Ar, therefore, does not become distributed evenly throughout the reactor. (C) 1998 American Vacuum Society. [S0734-2101(98)04604-1 ].