Field of the Invention
The invention relates to an apparatus for coating a substrate with thin layers from targets between which a gas discharge plasma is maintained in order to produce the ions necessary for the bombardment of targets connected to alternating current, the process chamber containing a gas under a certain partial pressure, and the targets are connected to a current source and being wired so that they form alternately the cathode and anode of the gas discharge.
Brief Description of the Prior Art
An apparatus is known for the reactive coating of a substrate (DE-A-41 36 655.7, addition to DE-A-40 42 289.5) in which a cathode consisting of two electrically separate parts and configured as a magnetron cathode, in which the target base with yoke and magnet is connected as the one part--with the interposition of a capacitance--to the negative pole of a direct-current voltage supply and the target as the other part is connected to the voltage supply with interposition of a choke and a resistance parallel to the latter, the target being connected through an additional capacitance to the plus pole of the power supply and to the anode which in turn is connected to ground--with interposition of a resistance, while in series with the low-induction capacitance an inductance is inserted into the branch line to the resistance and to the choke and the value of the resistance is typically between 2 k.OMEGA. and 10 k.OMEGA..
This older apparatus is so constructed that it suppresses most of the arcs occurring during the coating process, reduces the energy of the arcs and improves the reignition of the plasma after arcing.
In another older patent application (P 41 27 504.7) a circuit has also been created for extinguishing arcs in plasma apparatus for the purpose of permitting high coating rates even in the sputtering of difficult materials, such as SiO.sub.2, for example. The momentary value of the voltage of the plasma section is compared with a voltage which corresponds to an average plasma voltage obtained over a given period, and then, if the difference between the momentary value of the plasma voltage exceeds a given level, the plasma section is cut off from the voltage source.
In the reactive sputtering of metal oxides or metal nitride, the development of more or less good insulating properties on the target surface cannot be avoided. Such insulating coatings on the target are in plasma contact and therefore take on an electrical charge. On account of the high electrical field strengths in these thin coatings, electrical breakdowns occur. In this manner an arc is initialized. The consequences are a spot destruction of the target and thus coating defects on the substrate.
In medium-frequency sputtering (as described for example in DE-A-41 38 793 and DE-A-41 38 794) it has been found that spontaneous arcing occurs less frequently than in normal DC sputtering. The peculiarity of the known process is that the cathodes are reverse-charged periodically in step with the medium frequency.
Also known is an apparatus for coating a substrate, especially with electrically non-conductive coatings (DE-A-42 02 425), from an electrically conductive target in a reactive (e.g., oxidizing) atmosphere, consisting of a direct-current source which is connected to a cathode disposed in an evacuable coating chamber and including a magnet, which cooperates electrically with the target, which is sputtered and its sputtered particles deposit themselves on the substrate, an anode electrically separated from the sputtering chamber being provided, and a DC magnetron cathode connected to a DC current source can be brought for short time periods to a positive potential by means of a matched additional circuit, the frequency of this periodical pole reversal being variable according to the coating that is to be deposited.
Summary of the Invention
Setting out from the experience with apparatus for medium-frequency sputtering of thin coatings, the present invention is addressed to the problem of improving an apparatus of the type in question such that, in coating very large-area substrates, a strong and uniform ion bombardment will be achieved without the use of expensive power supplies, while the ion bombardment itself is to be controllable.
This problem is solved according to the invention by an apparatus in which the reversal of the direction of the current is performed through an H bridge formed by four switches, whose diagonal points are connected each with a magnetron cathode, each bearing a target, a line branching from the first conductor connecting the bridge with the first voltage source and connected with the positive pole of a voltage source or of a charge storage whose minus pole is connected by a fifth switch to the process chamber, and a second conductor connects the first voltage source to a choke and the choke is connected with a bridge, and all switches are operated by a control circuit in a periodic and adjustable mode.
In an alternative embodiment the reversing of the current direction is performed through an H bridge whose diagonal points are connected each with a magnetron cathode, each bearing a target, while a line branches from the first conductor joining the bridge to the first voltage source and is connected to the positive pole of a voltage source or charge storage means whose negative pole is connected to the process chamber via a fifth switch, and a second conductor connects the first voltage source with the bridge, while a second charge storage is connected to the first and second conductor, and all switches are operated by a control circuit in a regular and variable mode.
Additional details and features of the invention will become apparent from the specification herein.
Brief Description of the Drawings
The invention admits of a great variety of embodiments; four of them are represented in a purely schematic manner in the appended drawings, wherein:
FIG. 1 shows a greatly simplified block diagram of an apparatus of the kind in question;
FIG. 2 shows the current pattern of various phases of the circuit of FIG. 1;
FIGS. 3-5 show the electrical circuit diagram with an H bridge connected to a first power source and preceding the two electrodes, a second power source, and a choke in the neutral line of the bridge;
FIGS. 6-8 show a circuit similar to those in FIGS. 3 to 5, but with a capacitor inserted between the power line and negative pole;
FIGS. 9-11 show a circuit similar to that of FIGS. 6 to 8, but with a second power source in the form of a condenser; and
FIG. 12 shows a circuit similar to that of FIGS. 3 to 5 with a second power source configured as a condenser.
Detailed Description
The schematic diagram in FIG. 1 consists of a first power source 3, a vacuum chamber 6 with the electrodes 9 and 10 disposed therein with targets 12 and 13 and the substrate 24, a circuit 4 and a second power source 5. The conductor connected to the electrode 9 is connected by the circuit 4 and the line 21 to the second power source 5 and by switch 20 to the ground when the circuit 4 in phase II (see FIG. 2) short-circuits the power source 3.
The circuit according to FIGS. 3 to 5 consists of the generator 3, the bridge circuit 4 electrically connected to the latter, the second generator 5, the vacuum chamber 6 with vacuum pump 7, gas inlet valve 8, the two electrodes 9, 10, with corresponding targets 12, 13, the choke 11, the ground conductor 15 and the switches 16 to 20. During the sputtering process the IGBT switches 16 to 20 are operated by a control circuit, not shown, according to a regular and variable mode in the three phases represented in the drawings (FIGS. 3 to 5), so that the targets 12, 13 alternately form the cathode and anode of the gas discharge.
As FIG. 3 shows, the current flows from the generator 3 through the conductor 14 and the switch 19 to the electrode 10 with target 13, while the second power source 5 is uncoupled from the electrodes 12, 13, since the switch 20 inserted into the branch line 21, as well as switch 18 of the H bridge are open. The current is limited in this period by the choke 11 in the power supply.
In FIG. 4 is shown the next phase of the sputtering process, in which all of the switches 16 to 19 of the H bridge, and also switch 20, are closed. This pause period in the discharge is utilized in order to connect the two electrodes 9 and 10 by the switch 20 to an external power source 5. The duration of the pause, and thus the ion acceleration time, is selected such that the majority of the ions has covered the distance from the electrodes 9 and 10 to the substrate 24. Since the duration is also variable by the setting of the switches, both the energy through the external voltage source 5 and the number of ions can be selected by the timing.
The same circuit can also be made for a voltage pulser, like the one represented in FIGS. 6 to 8, in which case the corresponding circuit differs from those in FIGS. 1 to 3 in that the two conductors 14 and 23 are connected by a line 25 to a capacitor 26 inserted into the latter. Furthermore, the choke br limiting t he current in the embodiment according to FIGS. 1 to 3 is lacking.
FIGS. 9 to 11 show another variant, in which the external power source 5 is replaced with a condenser 29. During the sputtering period the condenser 29 is charged, and during the pauses the energy stored in the condenser 29 is used to accelerate the ions to the substrate 24. This variant limits the freedom of the acceleration voltage, but for some applications this makes possible a more economical construction. The negative pole of the first voltage source 3 is connected through a branch line 27 with switch 30 to the conductor 15 to the process chamber 6, and all the switches (16 to 19, 20, 28, 30) are operated by a control circuit in a regular and variable mode.
FIG. 12 shows the simplified circuit wit h the condenser 29 in the current pulser version.
To intensity the ion bombardment, known solutions make use either of separate ion sources, e.g., the APS, or a bias voltage in sputtering. While separate ion sources have their main disadvantage in the ion distribution, i.e., they are not selectable on large surfaces, the problem with bringing in a bias voltage consists, especially in the case of large glass surfaces, in installing high-frequency electrodes of large surface are a and corresponding powers. The said problems are the reason why no ion intensification has been used heretofore in large-area coating. In the conventional medium frequency discharge in the double magnetron system, a natural acceleration voltage establishes itself, which can be varied only within narrow limits depending on the other parameters. The range of variation is not sufficient for a great number of applications in which a drastic structural change is needed.
The solution offered by the invention, however, has the advantage that the acceleration voltage can be selected independently of other process parameters, so that for the first time certain coatings can now be produced on large areas.