TY - JOUR
T1 - Effects of discharge frequency in plasma etching and ultrahigh-frequency plasma source for high-performance etching for ultralarge-scale integrated circuits
AU - Samukawa, Seiji
AU - Donnelly, Vincent M.
AU - Malyshev, Mikhail V.
PY - 2000
Y1 - 2000
N2 - A low-temperature, uniform, high-density plasma is produced by applying ultrahigh-frequency (UHF) power through a spokewise antenna. The plasma is uniform within ±5% over a diameter of 30cm. No magnetic field is needed to maintain the high-density plasma. Consequently, the plasma source is fairly simple and lightweight. This plasma creates a high electron density and a low degree of dissociation of the feed gas at the same time because the electron energy distribution function is not Maxwellian (bi-Maxwellian distributions). The plasma characteristics are highly suitable for the precise etching of Al and gate electrodes. Additionally, by the combination of bi-Maxwellian electron energy distribution in the UHF plasma and new fluorocarbon gas chemistries (C2F4, CF3I), selective radical generations of CF2 and CF3 could be realized for high-aspect contact hole patterning of SiO2. A high ion density and a high-energy tail in the electron energy distribution can also be maintained over a wide range of pressure (from 3 to 20mTorr), whereas in conventional inductively coupled plasma (ICP: 13.56 MHz), the ion density and number of high-energy electrons are drastically reduced when the gas pressure is increased. This indicates that the ionization in the UHF plasma does not depend significantly on gas pressures between 3 and 20mTorr because the discharge frequency is higher than the frequency of electron collisions in the plasma. As a result, the UHF plasma provides a process window for high-performance etching that is wider than the one provided by an ICP.
AB - A low-temperature, uniform, high-density plasma is produced by applying ultrahigh-frequency (UHF) power through a spokewise antenna. The plasma is uniform within ±5% over a diameter of 30cm. No magnetic field is needed to maintain the high-density plasma. Consequently, the plasma source is fairly simple and lightweight. This plasma creates a high electron density and a low degree of dissociation of the feed gas at the same time because the electron energy distribution function is not Maxwellian (bi-Maxwellian distributions). The plasma characteristics are highly suitable for the precise etching of Al and gate electrodes. Additionally, by the combination of bi-Maxwellian electron energy distribution in the UHF plasma and new fluorocarbon gas chemistries (C2F4, CF3I), selective radical generations of CF2 and CF3 could be realized for high-aspect contact hole patterning of SiO2. A high ion density and a high-energy tail in the electron energy distribution can also be maintained over a wide range of pressure (from 3 to 20mTorr), whereas in conventional inductively coupled plasma (ICP: 13.56 MHz), the ion density and number of high-energy electrons are drastically reduced when the gas pressure is increased. This indicates that the ionization in the UHF plasma does not depend significantly on gas pressures between 3 and 20mTorr because the discharge frequency is higher than the frequency of electron collisions in the plasma. As a result, the UHF plasma provides a process window for high-performance etching that is wider than the one provided by an ICP.
KW - Discharge frequency
KW - Electron energy distribution function
KW - Inductively coupled plasma
KW - Plasma etching
KW - Ultrahigh-frequency plasma
UR - http://www.scopus.com/inward/record.url?scp=0141458421&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0141458421&partnerID=8YFLogxK
U2 - 10.1143/jjap.39.1583
DO - 10.1143/jjap.39.1583
M3 - Article
AN - SCOPUS:0141458421
SN - 0021-4922
VL - 39
SP - 1583
EP - 1596
JO - Japanese Journal of Applied Physics, Part 1: Regular Papers & Short Notes
JF - Japanese Journal of Applied Physics, Part 1: Regular Papers & Short Notes
IS - 4 A
ER -