COMPARISON OF ADVANCED PLASMA SOURCES FOR ETCHING APPLICATIONS .3. ION ENERGY-DISTRIBUTION FUNCTIONS FOR A HELICON AND A MULTIPOLE ELECTRON-CYCLOTRON-RESONANCE SOURCE
Gw. Gibson et al., COMPARISON OF ADVANCED PLASMA SOURCES FOR ETCHING APPLICATIONS .3. ION ENERGY-DISTRIBUTION FUNCTIONS FOR A HELICON AND A MULTIPOLE ELECTRON-CYCLOTRON-RESONANCE SOURCE, Journal of vacuum science & technology. B, Microelectronics and nanometer structures processing, measurement and phenomena, 12(4), 1994, pp. 2333-2341
As part of our research effort in evaluating the etching performance o
f high density plasma sources, we measured ion energy distribution fun
ctions near the wafer surface for a helicon and a multipole electron c
yclotron resonance source (ECR). The following two salient results sta
nd out: first is the remarkable similarity in behavior of the two sour
ces which was also observed in previous studies comparing etching rate
s, profile control, and Langmuir probe diagnostics; and second is the
surprising level of coupling between the applied rf bias and the bulk
plasma. For both sources, the ion flux increases strongly with source
power, decreases by 20%-40% as the reactor pressure increases from 2.0
to 5.0 mTorr, and is weakly modified by the applied rf bias. The mean
ion energy is strongly influenced by the applied rf-bias and is relat
ively insensitive to source power and pressure. The ion flux exhibits
high uniformity for both sources, with the helicon exhibiting slightly
better uniformity. However, we note that instabilities in the ECR dis
charge from mode jumps caused by different operating conditions and ch
anging reactor wall conditions, such as temperature, result in poorer
uniformity. The behavior of ions with respect to applied source and rf
-bias powers follows roughly the trends expected of quiescent, high de
nsity plasmas in contact with a rf-biased electrode (i.e., independent
control of ion flux and mean ion energy). However, there exist subtle
effects upon the ion flux, such as bimodal energy distributions, brou
ght about by the coupling of the rf-bias power into the bulk plasma. T
his coupling may be an essential parameter in wafer platen design that
must be addressed in order to obtain high etching rate uniformity.