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HCD-L 300
13,56 MHz
hollow cathode plasma source

Features:
- operation over an extended power and pressure range
- no mode jumps
- high plasma and radical species densities with excellent axial
homgeneity
- compatible with chemical reactive and non-reactive gases
- cw and pulsed power operation
- low contamination
- scaleable
Applications:
- plasma-enhanced chemical vapor deposition (PE-CVD)
- plasma polymerisation
- surface modification
- plasma cleaning
- plasma etching
- reactive and non-reactive ion etching
- basic reasearch in the material sciences
Hollow cathode discharges
represent a relatively simple means for
the efficient production of high density, low temperature plasmas.
The plasma source HCD L-300 employs the hollow cathode
effect. In principle, the HCD L-300 consists of two
cylindrical tubes aligned coaxially. The innner tube enclosing the plasma is rf powered;
the outer tube is electrically grounded. Along the cylindrical axis multiple holes are
drilled into the inner and outer cylinder allowing plasma jets to be extracted after the
primary plasma has been excited in the hollow cathode. A proprietary internal cathode
structure guaranties a homogeneous plasma jet formation over extended source lenghts.
The HCD L-300 extends over a length of 300 mm. By stacking
together two or three HCD L-300 total source lenghts are 600 (HCD L-600) and 900 mm (HCD L-900),
respectively.
Performance
There are two major parameters controlling the performance and
technical applicability of hollow cathode plasma sources such as the HCD L-300. These are the working pressure range of the hollow
cathode (primary) discharge and the rf power required for plasma breakdown, i.e.
ignition. Once the plasma is excited the rf power can be varied over an extended power and
pressure range without affecting the stability of the discharge and overall plasma jet
formation. When further reducing the rf power, there is a minimum where the plasma no
longer is stable.
Lifetime
The HCD L-300 is manufactured using
exclusively aluminum and ceramic parts for electrical insulation. No quartz windows etc.
are necessary. Since all ceramic parts are shielded from direct plasma interaction and
sputtering the source is extemly robust and offers extended lifetimes often superior to
those of inductively and microwave excited plasmas.
Technical data
Rf power (max): 300 W (air cooled)
1000 W (water cooled)
Frequency 13.56 MHz
pressure range: 5...1000 Pa
Gas flow rate: 5...300 sccm
Application note:
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