Chemistry: electrical and wave energy – Apparatus – Coating – forming or etching by sputtering
Reexamination Certificate
2001-04-23
2002-12-17
VerSteeg, Steven H. (Department: 1753)
Chemistry: electrical and wave energy
Apparatus
Coating, forming or etching by sputtering
C204S192110, C204S192120, C204S298030, C204S298040, C204S298110, C427S008000, C427S569000, C427S255500, C118S730000, C118S712000, C118S720000, C118S7230VE, C118S7230ER, C118S504000
Reexamination Certificate
active
06495010
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates generally to thin film deposition and etching systems. In particular, the present invention relates to methods and apparatus for depositing thin films with very high uniformity. The present invention also relates to methods and apparatus for etching material at highly uniform etch rates.
BACKGROUND OF THE INVENTION
There are three common techniques used to deposit thin films onto substrates. These techniques are evaporation, ion beam deposition, and magnetron sputtering. 
FIG. 1
 illustrates a schematic diagram of a prior art electron beam evaporation deposition system 
10
. The evaporation system 
10
 is enclosed in a vacuum chamber 
12
. An electron gun 
14
 generates an electron beam 
16
 that is used to heat a crucible 
18
 containing the deposition material to a temperature that causes the deposition material to evaporate. The electron beam is deflected with a magnet 
20
 that causes the electron beam to strike the desired location in the crucible 
18
. Typical evaporation systems have multiple crucibles.
Some Evaporation systems include multiple sources and multiple electron guns that produce deposition material from two or more sources and deposit the deposition material simultaneously onto a substrate. Alternatively, a thermal heating element (not shown) is used to heat the crucible 
18
. A substrate support 
22
 that typically supports multiple substrates 
23
 is positioned in the path of the evaporated material. In some known evaporation systems, the substrate support 
22
 is rotated with a motor 
24
 in order to increase the uniformity of the deposited thin film.
FIG. 2
 illustrates a schematic diagram of a prior art ion beam sputter deposition system 
50
. The ion beam sputter deposition system 
50
 is enclosed in a vacuum chamber 
52
. An ion source 
54
 generates an ion beam 
56
 that is directed to one or more targets 
58
. The ion beam 
56
 strikes the target 
58
 and sputters neutral atoms from the target 
58
 with a stutter flux 
60
. A substrate support 
62
 that typically supports multiple substrates 
64
 is positioned in the path of the sputter flux 
60
. The sputter flux 
60
 bombards the substrates, thereby depositing a sputtered thin film. In order to increase the uniformity of the sputtered thin film, the substrate support 
62
 may be rotated with a motor 
66
. Ion beam sputtering is advantageous because it permits independent control over the energy and current density of the bombarding ions.
FIG. 3
 illustrates a schematic diagram of a prior art magnetron sputter deposition system 
80
. The magnetron sputter deposition system 
80
 is enclosed in a vacuum chamber 
82
. The magnetron sputter deposition system 
80
 includes a diode device having an anode 
84
 and a cathode 
86
. A magnet 
88
 is positioned behind the cathode 
86
. Two ring-shaped cathodes and a disk-shaped anode are shown, but there are several other known configurations.
The cathode 
86
 is biased to a negative potential that is high enough to induce a breakdown in the surrounding gas and to sustain a plasma 
90
. The magnet 
88
 generates a magnetic field 
92
 behind the cathode 
86
 that traps electrons generated by the cathode 
86
. The electrons lose energy in spiral paths in the plasma 
90
 and are collected by the anode 
84
. The electrons enhance the bombarding efficiency of ions 
94
 in the plasma 
90
. Neutral atoms 
96
 are sputtered fit the cathode 
86
 with a sputter flux 
98
. The sputter flux 
98
 bombards the substrates 
64
, thereby depositing a sputtered thin film onto the substrate 
64
.
The substrates 
64
 in known systems are typically placed at a distance from the cathode 
86
 ranging between two and ten inches. In order to increase the uniformity of the sputtered film, the substrate support 
62
 may be rotated with a motor 
66
. Magnetron sputtering is advantageous because it has relatively high deposition rates, large deposition areas, and low substrate heating.
The deposition thickness uniformity achieved with these known techniques is limited by the flux uniformity achieved at the substrate plane and the type of substrate rotation. The flux uniformity can be adversely affected by target or deposition material imperfections that cause hot and cold spots, which affect the deposition rate. Typically, the flux uniformity changes with time. The flux uniformity can be improved somewhat by using a large target and/or by using a long distance from the target to the substrate. However, there are practical limits to the size of the target and the distance from the target to the substrate. Some applications, such as optical filters for high-speed optical communication systems, require thin film uniformities that cannot be achieved with these prior art techniques.
SUMMARY OF THE INVENTION
The present invention relates to methods and apparatus for depositing thin films using a differentially-pumped deposition source and deposition chamber, where the pressure in the deposition source is substantially higher than the pressure in the deposition chamber. The present invention also relates to methods and apparatus for using an ion source that generates an ion beam for ion beam assisted processing of the deposited thin films. In one embodiment, the ion beam and the deposition flux do not overlap and the ion beam is used for out-of-phase ion-beam-assisted processing. Both the deposition source and the ion beam source can be positioned a relatively short distance from the substrate, thereby exposing the substrate to a relatively high density of sputter flux and ion beam flux.
One embodiment of the deposition system of the present invention is a differentially-pumped magnetron sputtering system. The magnetron sputtering system has numerous advantages over known deposition systems. For example, the magnetron sputtering system deposits high purity, high-density films at high deposition rates with a high degree of uniformity and run-to-run consistency. In addition, the magnetron sputtering system has a long target lifetime and is relatively easy to maintain. Thin film uniformity can be improved by aperturing sputter flux from the sputter deposition source and then moving the substrates relative to the sputter flux with a dual-scan motion, such as a two dimensional motion. Thin film uniformity can also be improved by scanning one motion much faster than the other motion. Also, thin film uniformity can be improved by over-scanning.
Accordingly, the present invention features a differentially pumped deposition system that includes a deposition source that is positioned in a first chamber. In one embodiment, the deposition source is a magnetron sputter source. In another embodiment, the deposition source is an evaporation source. The deposition source generates deposition flux comprising neutral atoms and molecules.
A shield defines an aperture that is positioned in a path of the deposition flux. The shield passes the deposition flux through the aperture and substantially blocks the deposition flux from propagating past the shield everywhere else. The aperture may be shaped to increase the transmitted deposition flux. The aperture may also be shaped to reduce the over-scan area. A substrate support is positioned in a second chamber adjacent to the shield. The pressure in the second chamber is lower than the pressure in the first chamber.
The deposition system also includes a dual-scanning system that scans the substrate support relative to the aperture with a first and a second motion. The dual-scanning system may be a mechanical scanning system. The scan rate of the first motion. maybe substantially greater than the scan rate of the second motion The scan rate of at least one of the first motion and the second motion may also vary with time during deposition. In one embodiment the dual-scanning system comprises a rotational scanning system and a translational scanning system, wherein the first motion comprises a rotational motion having a rotation rate and the second motion comprises a translational motion having a translation rate. Th
Rauschenbach Kurt
Rauschenbach Patent Law Group
Unaxis USA Inc.
VerSteeg Steven H.
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