MICROWAVE PLASMA SOURCE DEVELOPMENT
In the late 1960's and the early 1970's plasma
etching was introduced as an alternative to "wet"-chemical
etching for integrated circuit (IC) manufacturing. Since then the
sophisticated process requirements for manufacturing microelectronic
devices have stimulated the continued development of plasma etching
technology. Today, plasma processing is an important enabling technology
for manufacturing computer chips and other electronic devices.
Fig 1: Cross section of MSU ECR reactor evaluated
by SEMATECH/SRC/Lucent Technologies for sub-0.35 micrometer polysilicon
gate etch[1].
Recently, modern plasma assisted etch process
requirements such as large-area, single-wafer, submicron, silicon
integrated circuit (IC) processing, and low-damage etching of electronic
and photonic structures have lead to the development of a new generation
of low-pressure, high-density plasma (HDP) sources. These plasma sources
must operate at low neutral pressures of 10-4 - 5 x 10-3
Torr, with high plasma densities of 1011 - 1012/cm3,
while still maintaining low plasma potentials. They must be capable of
uniformly etching 100-350 nanometer feature sizes over large surfaces,
must produce high process throughput and must provide an independent
substrate bias control of the ion energies. Current applications of these
HDP sources are large-area (200-300 millimeter diameters), submicron (0.13
- 0.30 micron) polysilicon etching for state-of-the-art computer chips and
dry etching for the fabrication of a large variety of III-V semiconductor
heterostructures and electro-optic devices.
MNEC engineers have invented
and developed a microwave excited HDP source. This source, which is shown
in Figure 1, sometimes is identified as a multipolar electron cyclotron
resonance (ECR) plasma source.
Fig 2: 0.25 micrometer profiles etched in
silicon.
It utilizes a tuned microwave cavity applicator that
efficiently couples microwave energy into a discharge volume inside a
quartz chamber. A multipolar static ECR magnetic field is impressed on the
discharge by rare-earth magnets equally spaced in a circle around and
adjacent to the quartz discharge chamber. A microwave discharge is formed
inside the quartz chamber and diffuses onto the large area silicon
substrate. An applied 13.56 MHz bias on the substrate provides an
independent adjustment of the ion energies before they strike the
substrate.
This HDP source can be built in many different sizes
ranging from a few to over 24 inches in diameter. It has been successfully
evaluated in single-wafer submicron polysilicon etching
(see Figure 2) and other etching applications such as the etching of III-V
and II-VI semiconductor heterostrucrues and electro-optic
devices (see Figure 3).
Fig 3: InGaAs/InGaP/InP quantum-well laser (top
disk: electrode and bottom disk: laser) courtesy of S. J. Pearton.
MNEC investigators have made numerous contributions
to the invention, the development, the application and the fundamental
understanding of these low-pressure ECR microwave plasma sources. See NSF
Grant - DMI 9713298, plasma etching and the References
for additional information on this plasma source technology and associated
MNEC faculty research activities.
References
High-density plasma source development
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Silicon etching
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Etching of III-V and II-VI semiconductors
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S.J. Pearton, C.R. Abernathy, R.F. Kopf, F. Ren, and W.S. Hobson,
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