Procedure and apparatus for the coating of materials by means of a pulsating plasma beam
The present invention relates to a procedure and an apparatus for the coating of materials.
Coatings consisting of or resembling a diamond material have properties similar to corresponding traditional dia¬ monds. The first property is hardness. Another significant mechanical property is a low friction coefficient. The resistance to wear is also extraordinary. Furthermore, such a coating remains unchanged in all known kinds of acid and base. Diamond and diamond-like materials are therefore e- specially suited for the coating of objects subject to wear or corrosion, e.g. bearings without lubrication. A further notable factor is the high refraction index of diamonds.
In microelectronics, the high thermal capacity and thermal conductivity of diamond and diamond-like coatings provide significant advantages. To achieve higher component densi¬ ties and speeds, it is necessary to reduce the structural size of integrated circuits. This makes it more difficult to remove the heat generated by the electric current, and it also means that good conductivity is more important than before.
In current practice, diamond-like coatings are produced by direct ion beam treatment, which is based on increasing the energy of ions. In direct ion beam coating, the coat is grown on the surface of the object material directly from the ion beam, from which the impurities have been removed by means of a separating magnet. The worst problem with this method is the difficulty of constructing an ion source of sufficient capacity. Another currently used method for growing a diamond coat is based on plasma-assisted vapour phase coat deposition (PAVCD) . In this method, a crystal¬ line diamond is grown from a mixture of methane and hydro¬ gen. Unlike the method based on the use of an energetic ion
beam for growing a diamond coat, which can be implemented in room temperature, the PAVCD method requires a high temperature of the order of 800°C. This is a serious disadvantage in view of the coating of conventional materials used in tools or construction.
The object of the present invention is to eliminate the drawbacks referred to above. The procedure of the invention for the coating of materials is characterized in that the material is coated using a pulsating plasma beam obtained from at least one electrode, said plasma beam being accelerated by a magnetic field and deflected by same to separate the uncharged particles from it, whereupon the plasma beam hits the surface of the material to be coated.
The advantages of the procedure are that it is simple and enables even large surfaces to be coated.
A preferred embodiment of the procedure of the invention is characterized in that the plasma beam consists of particles emitted from at least one electrode.
Another preferred embodiment of the procedure of the invention is characterized in that the coating is performed in a vacuum.
Another preferred embodiment of the procedure of the invention is characterized in that the coating process uses a gaseous medium which reacts with charged particles.
Another preferred embodiment of the procedure of the inven¬ tion is characterized in that the plasma beam is deflected by a magnetic field produced by means of a deflected coil.
The apparatus designed for implementing the procedure of the invention for the coating of materials is characterized in that, for the coating of a material, the apparatus is
provided with electrodes, at least one voltage source and at least one capacitor for producing a pulsating plasma beam and at least one deflected coil which generates a magnetic field that accelerates said plasma beam emitted by at least one electrode and deflects the beam to separate uncharged particles from it.
A preferred embodiment of the apparatus designed for imple¬ menting the procedure of the invention is characterized in that, to prevent oscillation of the voltage, the apparatus is provided with a diode connected in parallel with the capacitor.
Another preferred embodiment of the apparatus designed for implementing the procedure of the invention is character¬ ized in that it is provided with at least one igniter circuit to produce an arc between the electrodes.
Another preferred embodiment of the apparatus designed for implementing the procedure of the invention is character¬ ized in that at least one of the electrodes is of a cylindrical form.
Another preferred embodiment of the apparatus designed for implementing the procedure of the invention is character¬ ized in that at least one of the electrodes is placed wholly or partially inside the coil.
Another preferred embodiment of the apparatus designed for implementing the procedure of the invention is character¬ ized in that at least one of the electrodes is provided with at least one hole through which the plasma beam is directed.
Another preferred embodiment of the apparatus designed for implementing the procedure of the invention is character¬ ized in that the igniter circuit comprises a metal rod
inside each cylindrical electrode, another capacitor and a voltage source, which are used to produce an igniting arc between said electrode and said rod.
Another preferred embodiment of the apparatus designed for implementing the procedure of the invention is character¬ ized in that the igniter circuit has at least one external spark gap or switch.
In the following, the invention is described by the aid of an example with reference to the attached drawing, which represents a plasma accelerator and an object to be coated. For the coating of a material, the plasma accelerator pro¬ duces a cloud of plasma from carbon. This cloud is acceler¬ ated towards the object to be coated, and deflected by the magnetic field, whereupon the plasma beam strikes the sur¬ face of the object. Both the plasma accelerator and the ob¬ ject to be coated are placed in a vacuum. The plasma accel¬ erator has a cylindrical cathode 1 made of solid carbon, which is connected to the negative terminal of the first voltage source 2 and to the first terminal of the first capacitor C1. The disc-shaped anode 3, which has a hole in the middle, is connected to a cylindrical coil 4 formed from a copper conductor. The coil is deflected and connect¬ ed at one end to the positive terminal of the first voltage source 2 and to the other terminal of the first capacitor C1. Connected to the terminals of the capacitor C1 are also a diode D and a variable resistor R. The cathode 1 is partially and the anode 3 wholly inside the coil 4.
Inside the cathode 1 is a metal rod 5. The cathode 1 and the rod 5 together form a second voltage source 6 and, together with a second capacitor C2, an igniter circuit. The second voltage source 6 is variable. The cathode 1 is connected to the positive terminal of the second voltage source 6 and to the first terminal of the second capacitor C2. The metal rod 5 is connected to the negative terminal
of the second voltage source 6 and to the other terminal of the second capacitor C2.
The plasma accelerator performs the coating of a metal plate 7 as follows. The first voltage source 2 charges the first capacitor C1 , connected in parallel with the voltage source. The second voltage source 6 charges the second capacitor C2, likewise connected in parallel with it, until a spark-over occurs across the air gap between the cathode 1 and the metal rod 5, so that an arc is generated in said air gap. This arc discharges the second capacitor C2 and correspondingly produces an arc between the cathode 1 and the anode 3. As a result, the cathode begins to emit a beam of carbon particles consisting of charged ions and uncharged atoms. The arc between the cathode 1 and the anode 3 discharges the first capacitor C1 , and the arc is extinguished when the capacitor voltage falls below the level required for maintaining the arc. In this manner, a pulsating plasma beam is produced from carbon ions and carbon atoms. The duration of a pulse is determined by the capacitance of the first capacitor C1.
Connected in parallel with the first capacitor C1 are a diode D, whose function is to remove the reverse voltage produced across the first capacitor C1 by the oscillating circuit consisting of capacitor C1 and coil 4, and a variable resistor R protecting the diode D.
The plasma beam is accelerated through the magnetic field generated by the winding 4. Since the coil 4 has a curved shape, the charged ions passing through the hole 8 in the anode 3 will follow the curvature of the magnetic field, whereas uncharged particles will proceed straight past the plate 7. In this manner, uncharged particles are separated from the charged ions. The plate 7 to be coated is placed close to that end of the coil 4 which is connected to the first voltage source 2 and the first capacitor Cl . Since
the magnetic field generated by the coil 4 diverts the charged ions but does not affect the passage of uncharged particles, the plate to be coated is only struck by ions accelerated by the magnetic field.
When an ion with sufficient engergy, imparted by the mag¬ netic field, hits the surface of the plate 7, it is able to penetrate into the surface material. In the course of the next 10~tl s., the microscopic area around the penetrating ion undergoes remarkable changes. A significant proportion of the atoms in the plate surface have been displaced from their normal lattice positions, and the proportion of vacancies and intersitial atoms may reach a level of sever¬ al per cent. The conditions inside a cascade like this cor¬ respond to a temperature of several thousand °C, although the ambient temperature remains unchanged. Moreover, the pressure at the edges of the cascade increases. As a result of the process described, a diamond-like coat is produced on the surface of the plate 7.
Instead of a vacuum, it is also possible to use a gaseous medium which reacts with the ions in the surface of the material to be coated, producing e.g. a coat of boron nitride. In the igniter circuit, the arc between the cathode 1 and the metal rod 5 is automatically extinguished when the voltage across the second capacitor C2 falls below the level required for maintaining the arc. The igniter circuit may also employ an external spark gap 9 or switch to extinguish the arc between the cathode 1 and the metal rod 5 at a desired moment.
It is obvious to a person skilled in the art that different embodiments of the invention are not restricted to the examples described above, but that they may instead be varied within the scope of the following claims.